Prove2Me
Navigate
DiscoverCollectionsFormalpediaBlogsUsersMomentumMy Missions+
Prove2Me
⌕
Log in

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

Random Matrix Theory

61 missions · 27 completed

Missions

Open34Completed27All61
Machine LearningProbabilityStatistics·Captain: mikedeng1

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
10 thms4 active users
Linear algebraMachine LearningNumerical Analysis+2·Captain: mikedeng1

An Introduction to Matrix Concentration Inequalities III: A Matrix Sampling Estimator Satisfies E‖R̄ₙ − B‖ ≤ √(2m₂(R)log(d₁ + d₂)/n) + 2L log(d₁ + d₂)/(3n)Textbook

Motivation

Matrix approximation replaces a large or complicated matrix with a random matrix that is easier to store or compute. Averaging independent realizations improves accuracy while retaining the structure of each realization. Examples in Tropp's monograph include sparse approximations and randomized matrix products. The practical question is how the number of samples, the size of one sample, and its second moment control the spectral norm error. Tropp, §6.2

The book proves a matrix Bernstein inequality in Theorem 6.1.1, then applies it to an empirical matrix average in Corollary 6.2.1. Theorem 6.1.1 is already posed as TroppMatrixConcentration.matrix_bernstein on Prove2Me and is currently Open. This mission records the application with its own hypotheses and constants. The capstone concerns the estimator that a reader would construct, rather than a sum of abstract centered summands. Tropp, §§6.1–6.2

Setting

Let BBB be a fixed complex d1×d2d_1\times d_2d1​×d2​ matrix. A sample matrix RRR has the same size, has expectation BBB, and has spectral norm at most LLL almost surely. The equality ER=B\mathbb ER=BER=B makes one sample an unbiased estimate of BBB. The almost-sure bound limits the size of every sample except on a probability-zero set. The dimensions d1,d2d_1,d_2d1​,d2​ are positive integers, and nnn is a positive sample count.

Take independent copies R1,…,RnR_1,\ldots,R_nR1​,…,Rn​ with the distribution of RRR. Their matrix sampling estimator is

R‾n=1n∑k=1nRk.\overline R_n=\frac1n\sum_{k=1}^nR_k.Rn​=n1​k=1∑n​Rk​.

For any rectangular matrix AAA, A∗A^*A∗ denotes its conjugate transpose and ∥A∥\|A\|∥A∥ its spectral norm. The per-sample second moment is

m2(R)=max⁡{∥E(RR∗)∥,∥E(R∗R)∥}.m_2(R)=\max\{\|\mathbb E(RR^*)\|,\|\mathbb E(R^*R)\|\}.m2​(R)=max{∥E(RR∗)∥,∥E(R∗R)∥}.

Both terms matter for a rectangular matrix: RR∗RR^*RR∗ and R∗RR^*RR∗R act on different coordinate spaces. All expectations of matrices are entrywise expectations, represented by Bochner integrals in Lean. The almost-sure norm bound guarantees the moments used here are finite. Tropp, equations (6.2.4)–(6.2.6)

Formalization targets

Empirical matrix approximation

Corollary 6.2.1 gives an expectation estimate and a tail estimate for the same estimator. For every real t≥0t\ge0t≥0,

E∥R‾n−B∥≤2m2(R)log⁡(d1+d2)n+2Llog⁡(d1+d2)3n,\mathbb E\|\overline R_n-B\|\le \sqrt{\frac{2m_2(R)\log(d_1+d_2)}{n}}+ \frac{2L\log(d_1+d_2)}{3n},E∥Rn​−B∥≤n2m2​(R)log(d1​+d2​)​​+3n2Llog(d1​+d2​)​, P{∥R‾n−B∥≥t}≤(d1+d2)exp⁡(−nt2/2m2(R)+2Lt/3).\mathbb P\{\|\overline R_n-B\|\ge t\}\le (d_1+d_2)\exp\left(\frac{-nt^2/2}{m_2(R)+2Lt/3}\right).P{∥Rn​−B∥≥t}≤(d1​+d2​)exp(m2​(R)+2Lt/3−nt2/2​).

The goal includes both bounds. The expectation estimate controls average error; the tail estimate controls the chance of an error above a chosen threshold. The dimension enters only through log⁡(d1+d2)\log(d_1+d_2)log(d1​+d2​) in the expectation bound and the factor d1+d2d_1+d_2d1​+d2​ in the tail bound. These are the book's constants, including the factors 222 and 333 in the linear terms. Tropp, Corollary 6.2.1, p. 81

Supporting statements

The milestone list follows Corollary 6.1.2 for uncentered summands, the bound ∥n−1(Rk−B)∥≤2L/n\|n^{-1}(R_k-B)\|\le2L/n∥n−1(Rk​−B)∥≤2L/n, and the variance estimate v(R‾n−B)≤m2(R)/nv(\overline R_n-B)\le m_2(R)/nv(Rn​−B)≤m2​(R)/n. Equation (6.2.7) is a companion: a stated lower bound on nnn implies E∥R‾n−B∥≤2ε\mathbb E\|\overline R_n-B\|\le2\varepsilonE∥Rn​−B∥≤2ε for ε>0\varepsilon>0ε>0. Tropp, pp. 77, 82

Significance

The result turns a bound on one random matrix into a quantitative guarantee for an empirical approximation. It lets a user choose a sample count for a target error and evaluate both average error and failure probability. The same framework is instantiated later in the monograph for matrix sparsification and multiplication; those applications depend on controlling LLL and m2(R)m_2(R)m2​(R) for their particular sampling laws. Tropp, §§6.2–6.4

This is a known mathematical result proved in the book. Its Lean statement is an open formalization target. The mission adds a reusable empirical-mean definition and application statements built on the already published matrix spectral norm and rectangular second-moment definitions. A proof of the general matrix Bernstein theorem remains separate; the mission can draw on it when that platform theorem is proved.

Difficulty

The estimator error is a centered sum, but the sampling assumptions are given for an uncentered random matrix RRR. Bounding the centered summands changes the uniform bound from LLL to 2L/n2L/n2L/n. The variance parameter must be related to the second moment of one uncentered sample, with the correct 1/n1/n1/n scaling. Dropping the common-distribution condition would leave no relation between the samples' second moments and m2(R)m_2(R)m2​(R). Applying scalar concentration to entries would not directly give the stated spectral norm bound or its dimension dependence. Tropp, proof of Corollary 6.2.1, p. 82

Formalization scope

Matrices are Matrix (Fin d₁) (Fin d₂) ℂ. The spectral norm and rectSecondMoment are imported from tc's published TroppMatrixConcentration definitions. An arbitrary probability space carries a measurable reference matrix R0R_0R0​ and a finite family RkR_kRk​; iIndepFun expresses independence and IdentDistrib expresses equality in law with R0R_0R0​. The estimator is the finite sum scaled by n−1n^{-1}n−1. No particular sampling scheme or deterministic choice of RRR is fixed: the formal goal requires only the source's unbiasedness and boundedness conditions.

The Lean statements explicitly require d1,d2≥1d_1,d_2\ge1d1​,d2​≥1, n>0n>0n>0, measurability, and the almost-sure form of ∥R∥≤L\|R\|\le L∥R∥≤L. These make the logarithm and inverse sample count meaningful and make the random matrix laws well behaved. For the uncentered Bernstein corollary, integrability of each SkS_kSk​ is explicit because a bounded deviation from an unspecified mean alone does not establish that the mean exists. The goal also asserts integrability of its error norm, preventing a Bochner integral from silently taking Lean's default value for a nonintegrable function. The bound on RRR supplies that integrability. When the denominator in a tail formula is zero, the displayed total real division gives a loose bound at the degenerate case; the source's probabilistic claim remains valid.

Contributions that formalize the centered-summand calculation, the variance estimate, or the transfer from the general matrix Bernstein theorem are within scope. The imported matrix and probability definitions are reusable in other matrix concentration missions. The local empirical-mean definition is reusable whenever a matrix estimator averages finitely many random samples.

Selected references

  • Joel A. Tropp, An Introduction to Matrix Concentration Inequalities, Foundations and Trends in Machine Learning 8(1–2), 2015, arXiv:1501.01571v1, especially §§6.1–6.4.
7 thms3 active usersReviewed
AnalysisLinear algebraProbability·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices V: The Matrix Azuma Inequality for Adapted Sequences with Semidefinite Bounds on the Squared DifferencesResearch Paper

Motivation

Sums of random matrices appear throughout numerical linear algebra, statistics, combinatorics and quantum information: randomized sketching and sparsification, covariance estimation, graph sparsifiers, and the analysis of random features all reduce to controlling the largest eigenvalue of a sum of random self-adjoint matrices. Scalar concentration inequalities (Chernoff, Hoeffding, Bernstein, Azuma) have matrix analogues, and J. A. Tropp's User-Friendly Tail Bounds for Sums of Random Matrices (arXiv:1004.4389v7, Found. Comput. Math. 12 (2012) 389–434, doi:10.1007/s10208-011-9099-z) gives a unified derivation of them with explicit constants.

Many applications do not have independent summands: adaptive algorithms, online learning and sequential estimation produce sums whose terms depend on the past. The scalar tool for such sums is Azuma's inequality for martingales with bounded differences, and its corollary, McDiarmid's bounded differences inequality (McDiarmid 1998). This mission is the fifth of a series formalizing Tropp's paper; it targets §7, the matrix Azuma inequality.

Timeline. Ahlswede and Winter (2002) introduced a matrix analogue of the Laplace transform bound for independent sums; Oliveira (2010) gave the variant used in this paper. Tropp (this paper, 2010–2012) proved the matrix Azuma and McDiarmid inequalities below. More refined matrix martingale inequalities appear in Oliveira (2010) and in Tropp's Freedman's inequality for matrix martingales (2011), which the paper cites (p. 27) as requiring additional machinery.

Setting

All matrices are d×dd\times dd×d with complex entries, d≥1d\ge 1d≥1. A matrix is self-adjoint (s.a.) when it is Hermitian. For s.a. AAA, λmax⁡(A)\lambda_{\max}(A)λmax​(A) is its largest eigenvalue and ∥A∥\|A\|∥A∥ its spectral norm. Functions of s.a. matrices are defined spectrally: if A=QΛQ∗A=Q\Lambda Q^*A=QΛQ∗ then eA=QeΛQ∗e^{A}=Qe^{\Lambda}Q^*eA=QeΛQ∗, and log⁡\loglog is defined the same way on positive-definite matrices. A⪯BA\preceq BA⪯B is the semidefinite order: B−AB-AB−A is positive semidefinite.

Let (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) be a probability space with a filtration F0⊂F1⊂⋯⊂F\mathcal F_0\subset\mathcal F_1\subset\cdots\subset\mathcal FF0​⊂F1​⊂⋯⊂F, and write Ek[ ⋅ ]=E[ ⋅∣Fk]\mathbb E_k[\,\cdot\,]=\mathbb E[\,\cdot\mid\mathcal F_k]Ek​[⋅]=E[⋅∣Fk​]. The expectation and the conditional expectation of a random matrix are taken entrywise. A sequence X1,…,XnX_1,\dots,X_nX1​,…,Xn​ of random matrices is adapted when each XkX_kXk​ is Fk\mathcal F_kFk​-measurable. A matrix martingale is an adapted sequence of s.a. matrices YkY_kYk​ with E∥Yk∥<∞\mathbb E\|Y_k\|<\inftyE∥Yk​∥<∞ and Ek−1Yk=Yk−1\mathbb E_{k-1}Y_k=Y_{k-1}Ek−1​Yk​=Yk−1​; its difference sequence Xk=Yk−Yk−1X_k=Y_k-Y_{k-1}Xk​=Yk​−Yk−1​ satisfies Ek−1Xk=0\mathbb E_{k-1}X_k=0Ek−1​Xk​=0.

The hypotheses of the main theorem are: X1,…,XnX_1,\dots,X_nX1​,…,Xn​ is an adapted sequence of random s.a. matrices, and A1,…,AnA_1,\dots,A_nA1​,…,An​ is a fixed (non-random) sequence of s.a. matrices, with

Ek−1Xk=0andXk2⪯Ak2  almost surely.\mathbb E_{k-1}X_k = 0 \qquad\text{and}\qquad X_k^2\preceq A_k^2\ \text{ almost surely.}Ek−1​Xk​=0andXk2​⪯Ak2​  almost surely.

The variance parameter is σ2:=∥∑kAk2∥\sigma^2 := \big\|\sum_k A_k^2\big\|σ2:=​∑k​Ak2​​.

Formalization targets

Goal: Theorem 7.1 (Matrix Azuma), p. 27

For all t≥0t\ge 0t≥0,

P{λmax⁡(∑kXk)≥t}≤d⋅e−t2/8σ2.\mathbb P\Big\{\lambda_{\max}\Big(\sum_{k}X_k\Big)\ge t\Big\}\le d\cdot e^{-t^2/8\sigma^2}.P{λmax​(k∑​Xk​)≥t}≤d⋅e−t2/8σ2.

Milestones

In the order they are used:

  1. Display (2.6), Golden–Thompson: tr⁡eA+H≤tr⁡(eAeH)\operatorname{tr}e^{A+H}\le\operatorname{tr}(e^Ae^H)treA+H≤tr(eAeH) for s.a. A,HA,HA,H.
  2. Proposition 3.1, the Laplace transform method: P{λmax⁡(Y)≥t}≤inf⁡θ>0e−θt Etr⁡eθY\mathbb P\{\lambda_{\max}(Y)\ge t\}\le\inf_{\theta>0}e^{-\theta t}\,\mathbb E\operatorname{tr}e^{\theta Y}P{λmax​(Y)≥t}≤infθ>0​e−θtEtreθY.
  3. Corollary 3.3: Etr⁡exp⁡(H+X)≤tr⁡exp⁡(H+log⁡EeX)\mathbb E\operatorname{tr}\exp(H+X)\le\operatorname{tr}\exp(H+\log\mathbb E e^{X})Etrexp(H+X)≤trexp(H+logEeX).
  4. Lemma 4.3, Rademacher half: EeεθA⪯eθ2A2/2\mathbb E e^{\varepsilon\theta A}\preceq e^{\theta^2A^2/2}EeεθA⪯eθ2A2/2.
  5. Lemma 7.6 (Symmetrization): Etr⁡eH+X≤Etr⁡eH+2εX\mathbb E\operatorname{tr}e^{H+X}\le\mathbb E\operatorname{tr}e^{H+2\varepsilon X}EtreH+X≤EtreH+2εX when EX=0\mathbb EX=0EX=0 and ε\varepsilonε is an independent Rademacher variable.
  6. Lemma 7.7 (Azuma cgf): log⁡E[e2εθX∣X]⪯2θ2A2\log\mathbb E[e^{2\varepsilon\theta X}\mid X]\preceq2\theta^2A^2logE[e2εθX∣X]⪯2θ2A2 when X2⪯A2X^2\preceq A^2X2⪯A2.
  7. Display (7.5): Etr⁡exp⁡(∑kθXk)≤tr⁡exp⁡(2θ2∑kAk2)\mathbb E\operatorname{tr}\exp(\sum_k\theta X_k)\le\operatorname{tr}\exp(2\theta^2\sum_kA_k^2)Etrexp(∑k​θXk​)≤trexp(2θ2∑k​Ak2​) under the hypotheses of the goal.

Further statements

Corollary 7.2 is the martingale form, P{λmax⁡(Yn−EYn)≥t}≤d e−t2/8σ2\mathbb P\{\lambda_{\max}(Y_n-\mathbb EY_n)\ge t\}\le d\,e^{-t^2/8\sigma^2}P{λmax​(Yn​−EYn​)≥t}≤de−t2/8σ2. Corollary 7.5 (Matrix Bounded Differences) is the matrix McDiarmid inequality, P{λmax⁡(H(z)−EH(z))≥t}≤d e−t2/8σ2\mathbb P\{\lambda_{\max}(H(z)-\mathbb EH(z))\ge t\}\le d\,e^{-t^2/8\sigma^2}P{λmax​(H(z)−EH(z))≥t}≤de−t2/8σ2 for a matrix-valued function HHH of independent variables whose changes in one coordinate kkk have squares bounded by Ak2A_k^2Ak2​.

Significance

The result. The bound has the scalar subgaussian shape with two matrix features: a dimensional factor ddd, and a variance parameter equal to the norm of the sum ∑kAk2\sum_kA_k^2∑k​Ak2​ rather than the sum of the norms ∑k∥Ak∥2\sum_k\|A_k\|^2∑k​∥Ak​∥2. In the commuting case the two coincide; in general the first can be smaller by a factor of up to nnn. The theorem needs no independence, so it covers adapted constructions such as Doob martingales. Corollary 7.5, obtained from it, is the standard matrix tool for concentration of matrix-valued functions of independent data. With independent summands the theorem gives a matrix Hoeffding inequality (Theorem 1.3 of the paper).

Formalizing it. The result is proved in the paper; none of it is formalized. Mathlib has the continuous functional calculus, conditional expectation and filtrations, but no Golden–Thompson inequality, no Lieb concavity theorem, and no matrix tail inequality. A formalization produces a machine-checked matrix Azuma inequality, the Golden–Thompson inequality, and a symmetrization lemma for the trace exponential, all of which have uses beyond this paper.

Difficulty

The scalar proof of Azuma's inequality multiplies conditional moment generating functions, Eeθ∑Xk=E[eθ∑k<nXk En−1eθXn]\mathbb E e^{\theta\sum X_k}=\mathbb E\big[e^{\theta\sum_{k<n}X_k}\,\mathbb E_{n-1}e^{\theta X_n}\big]Eeθ∑Xk​=E[eθ∑k<n​Xk​En−1​eθXn​], and bounds each factor. For matrices this fails: eA+B≠eAeBe^{A+B}\neq e^Ae^BeA+B=eAeB unless AAA and BBB commute, and tr⁡eA+B+C≤tr⁡(eAeBeC)\operatorname{tr}e^{A+B+C}\le\operatorname{tr}(e^Ae^Be^C)treA+B+C≤tr(eAeBeC) is false, so the Golden–Thompson inequality cannot be iterated over nnn terms. The paper itself notes (p. 28) that the classical approach does not seem to extend. A second obstacle is that the hypothesis Xk2⪯Ak2X_k^2\preceq A_k^2Xk2​⪯Ak2​ bounds squares, not the matrices themselves; it does not give Xk⪯AkX_k\preceq A_kXk​⪯Ak​, so the scalar Hoeffding lemma for bounded centred variables has no direct matrix analogue. The infrastructure is also heavy: Lieb's concavity theorem underlies Corollary 3.3, and operator monotonicity of the logarithm is needed.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ, self-adjointness is IsHermitian, and ⪯\preceq⪯ is Mathlib's order under MatrixOrder. Matrix exponential and logarithm are cfc Real.exp and cfc Real.log. λmax⁡\lambda_{\max}λmax​ is the supremum of the real spectrum, which is why d≥1d\ge1d≥1 is assumed (NeZero d). Expectation and conditional expectation of matrices are entrywise Bochner integrals; adaptedness is entrywise strong measurability with respect to a Mathlib Filtration ℕ. The summands are indexed by k=1,…,nk=1,\dots,nk=1,…,n, so Fk−1\mathcal F_{k-1}Fk−1​ is never truncated. The bound Xk2⪯Ak2X_k^2\preceq A_k^2Xk2​⪯Ak2​ is required almost surely. The bounds AkA_kAk​ are deterministic matrices. The infimum over θ>0\theta>0θ>0 in Proposition 3.1 is posed as the bound for each θ>0\theta>0θ>0 at which the expectation is finite.

The hypotheses must not be made vacuous. Integrability of each XkX_kXk​ is assumed explicitly, because for a non-integrable variable Lean's conditional expectation is 000 and the centring hypothesis would say nothing. The XkX_kXk​ are not assumed independent: an independence hypothesis would turn the goal into the weaker matrix Hoeffding inequality.

Two readings are recorded in the statements. In Lemma 7.7 the conditional expectation given XXX is replaced by the expectation over ε\varepsilonε at each fixed value xxx with x2⪯A2x^2\preceq A^2x2⪯A2; by independence these agree. Corollary 7.2 adds the hypothesis that Y0Y_0Y0​ is almost surely constant, without which Yn−EYn≠∑kXkY_n-\mathbb EY_n\neq\sum_kX_kYn​−EYn​=∑k​Xk​.

A complete development needs: Golden–Thompson; Lieb's concavity theorem (or Corollary 3.3 directly); operator monotonicity of the matrix logarithm; monotonicity of the trace exponential; conditional expectation of matrix-valued variables and its interaction with the semidefinite order. All of these are reusable well beyond this mission, and contributions of any of them are welcome. Proposition 3.1, Corollary 3.3 and Lemma 4.3 are also milestones of other missions in this series.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, Found. Comput. Math. 12 (2012) 389–434; cited version arXiv:1004.4389v7 (2011). https://arxiv.org/abs/1004.4389v7
  • R. Ahlswede and A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48 (2002) 569–579. https://doi.org/10.1109/18.985947
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
  • J. A. Tropp, Freedman's inequality for matrix martingales, Electron. Commun. Probab. 16 (2011) 262–270. https://arxiv.org/abs/1101.3039
  • R. I. Oliveira, Concentration of the adjacency matrix and of the Laplacian in random graphs with independent edges, arXiv:0911.0600 (2010). https://arxiv.org/abs/0911.0600
  • C. McDiarmid, Concentration, in Probabilistic Methods for Algorithmic Discrete Mathematics, Springer (1998) 195–248. https://doi.org/10.1007/978-3-662-12788-9_6
  • R. Bhatia, Matrix Analysis, Springer GTM 169 (1997), Sec. IX.3. https://doi.org/10.1007/978-1-4612-0653-8
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
10 thms3 active usersReviewed
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
17 thms3 active usersReviewed
Machine LearningOptimizationStatistics·Captain: mikedeng1

Nonconvex Low-Rank Tensor Completion from Noisy Data: Spectrally Initialized Vanilla Gradient Descent Recovers the Tensor Factors at a Linear Rate to Near-Optimal ℓ2 and ℓ2,∞ AccuracyResearch Paper

Motivation

A partially observed array with three indices appears when data record relationships among triples of objects. If its entries have a low-rank structure, one can hope to recover the full array from far fewer than d3d^3d3 measurements. Cai, Li, Poor and Chen study this problem when the measurements are noisy and only a random subset of entries is seen. Their result gives a statistical error bound for a concrete two-stage method: spectral initialization followed by ordinary gradient descent on a nonconvex loss. It is a known theorem, proved in the pinned preprint, rather than an open conjecture.

Setting

The unknown symmetric order-three tensor is T⋆∈Rd×d×dT^\star\in\mathbb R^{d\times d\times d}T⋆∈Rd×d×d. It has a CP decomposition T⋆=∑s=1r(us⋆)⊗3T^\star=\sum_{s=1}^r(u_s^\star)^{\otimes3}T⋆=∑s=1r​(us⋆​)⊗3, where the nonzero columns us⋆u_s^\starus⋆​ form U⋆∈Rd×rU^\star\in\mathbb R^{d\times r}U⋆∈Rd×r. Each unordered triple of coordinates is sampled independently with probability ppp; its six permutations share one sampling decision. On a sampled triple the observation is Tijk⋆+EijkT^\star_{ijk}+E_{ijk}Tijk⋆​+Eijk​, with symmetric, centered, independent sub-Gaussian noise of variance at most σ2\sigma^2σ2. The observed tensor TTT vanishes outside the sampled set Ω\OmegaΩ.

For a candidate factor matrix U=[u1,…,ur]U=[u_1,\ldots,u_r]U=[u1​,…,ur​], the objective is

f(U)=16p∥PΩ ⁣(∑s=1rus⊗3−T)∥F2.f(U)=\frac{1}{6p}\left\|P_\Omega\!\left(\sum_{s=1}^r u_s^{\otimes3}-T\right)\right\|_F^2.f(U)=6p1​​PΩ​(s=1∑r​us⊗3​−T)​F2​.

Algorithm 2 obtains a leading rrr-dimensional eigenspace from an off-diagonal Gram matrix of the mode-one unfolding of p−1Tp^{-1}Tp−1T. Algorithm 3 uses Gaussian restarts, leading singular vectors, and greedy pruning to turn that subspace into a factor matrix U0U^0U0. Algorithm 1 then applies the gradient step to fff. Eigenvalue ties, leading singular-vector choices, and pruning ties can produce several admissible executions; the result concerns every execution.

Incoherence μ\muμ measures how evenly the tensor and factors spread across coordinates and how nearly orthogonal distinct factors are. The condition number κ\kappaκ is the ratio of the largest to smallest factor norm. Write λmin⁡⋆=min⁡s∥us⋆∥23\lambda^\star_{\min}=\min_s\|u_s^\star\|_2^3λmin⋆​=mins​∥us⋆​∥23​ and λmax⁡⋆=max⁡s∥us⋆∥23\lambda^\star_{\max}=\max_s\|u_s^\star\|_2^3λmax⋆​=maxs​∥us⋆​∥23​. Distances dist⁡F\operatorname{dist}_FdistF​, dist⁡∞\operatorname{dist}_\inftydist∞​, and dist⁡2,∞\operatorname{dist}_{2,\infty}dist2,∞​ minimize their respective matrix norms over permutations of the rrr columns.

Formalization targets

The goal is Theorem 2.4, in the bounded-rank, bounded-incoherence, bounded-condition-number regime. Under its printed sampling, noise, restart, threshold and step-size conditions, for every 0≤t≤d50\le t\le d^50≤t≤d5 it asserts, with probability at least 1−δ1-\delta1−δ,

dist⁡F(Ut,U⋆)≤(C1ρt+C2σλmin⁡⋆dlog⁡dp)∥U⋆∥F,\operatorname{dist}_F(U^t,U^\star)\le\left(C_1\rho^t+C_2\frac{\sigma}{\lambda^\star_{\min}}\sqrt{\frac{d\log d}{p}}\right)\|U^\star\|_F,distF​(Ut,U⋆)≤(C1​ρt+C2​λmin⋆​σ​pdlogd​​)∥U⋆∥F​, dist⁡∞(Ut,U⋆)≤dist⁡2,∞(Ut,U⋆)≤(C3ρt+C4σλmin⁡⋆dlog⁡dp)∥U⋆∥2,∞.\operatorname{dist}_\infty(U^t,U^\star)\le\operatorname{dist}_{2,\infty}(U^t,U^\star)\le\left(C_3\rho^t+C_4\frac{\sigma}{\lambda^\star_{\min}}\sqrt{\frac{d\log d}{p}}\right)\|U^\star\|_{2,\infty}.dist∞​(Ut,U⋆)≤dist2,∞​(Ut,U⋆)≤(C3​ρt+C4​λmin⋆​σ​pdlogd​​)∥U⋆∥2,∞​.

The rate is fixed to ρ=1−λmin⁡⋆,4/3η/5\rho=1-\lambda_{\min}^{\star,4/3}\eta/5ρ=1−λmin⋆,4/3​η/5, consistent with the paper's local-convergence lemmas. Milestones formalize the gradient identity (36), local Hessian bounds (Lemma 5.1), spectral-subspace recovery (Lemma 5.7), factor retrieval (Theorem 5.9), and the paper's general-parameter recovery theorem (Theorem 2.8). The latter makes the dependence on μ\muμ and rrr explicit.

Significance

The inequalities give two guarantees at once: geometric reduction of initialization error and an explicit noise floor. The 2,∞2,\infty2,∞ bound controls the error in each coordinate row, which a Frobenius estimate alone does not supply. Together with the tensor-entry corollaries in the paper, they explain the accuracy of this practical nonconvex method under random subsampling. The authors also specify how the sample probability, noise level, rank and incoherence interact, so the result can be compared to other tensor-completion methods.

This mission asks for a machine-checked version of the known result. Its published ψ₂ norm definition is reused; the paper-specific tensor model, spectral initialization relations, loss and gradient iteration are new. The theorem statements compile with sorry, so none of their proofs is claimed as machine checked here. Proofs of the listed milestones, the main theorem, and faithful auxiliary concentration results are welcome; the paper's numerical experiments are outside this formalization.

Difficulty

The gradient loss is nonconvex, so global convexity cannot justify the iteration bound. The local Hessian estimate applies only near U⋆U^\starU⋆ in both Frobenius and rowwise norm. A Frobenius estimate alone cannot establish the rowwise condition at every iteration. The spectral initializer must also select individual factors from a subspace despite nearly tied eigenvalues and noisy tensor contractions. These are the points where a direct appeal to standard smooth-gradient-descent theory stops short of the stated result.

Formalization scope

Coordinates are Fin d and Fin r, with zero-based indexing; the PDF uses one-based indices. All logarithms are natural. Tensor and matrix norms are explicit finite-coordinate Euclidean norms. Minima over permutations range over all permutations of Fin r, and maxima in the incoherence parameters range over the indices specified by Definition 2.1. Sampling is on sorted triples, then extended by symmetry. The probability model is a single probability space carrying the sampling indicators, noise variables and Gaussian restarts, jointly independent; the paper leaves some cross-family independence implicit. Noise has mean zero, variance at most σ2\sigma^2σ2, and ψ₂ norm at most σ\sigmaσ using the published extended-nonnegative norm. The last bound makes the paper's sub-Gaussian scale explicit.

The statements use d≥d0≥2d\ge d_0\ge2d≥d0​≥2, r≥1r\ge1r≥1, nonzero true factor columns, 0<p≤10<p\le10<p≤1, and σ≥0\sigma\ge0σ≥0. Theorems 2.8 and 5.9 use r≥2r\ge2r≥2 and round their real-valued restart count up to a natural number; this handles the boundary where log⁡r=0\log r=0logr=0. Theorem 2.4 places its claimed absolute error constants before the rank and incoherence bounds and all instance data. Probability is expressed as the outer measure of the bad event, since admissible-execution predicates quantify over choices and need not be measurable. Each good event explicitly asserts that an admissible execution exists before requiring the bounds for every execution; otherwise a failed pruning run would make a universal claim vacuous.

The remaining reusable infrastructure includes concentration for symmetric sampled tensors, finite-dimensional spectral perturbation with ties, and derivative estimates for the cubic factor map. The paper's leave-one-out iteration lemmas and their auxiliary estimators are not included in this initial milestone list; they remain natural contributions toward the full proof.

Selected references

  • C. Cai, G. Li, H. V. Poor and Y. Chen, Nonconvex Low-Rank Tensor Completion from Noisy Data, arXiv:1911.04436v2, 2021; published in Operations Research 70(2), 2022. Preprint.
  • R. Vershynin, High-Dimensional Probability: An Introduction with Applications in Data Science, Cambridge University Press, 2018, Definition 2.5.6 for the ψ₂ norm. Publisher DOI.
8 thms2 active usersReviewed
Convex OptimizationStatistics·Captain: mikedeng1

Noisy Matrix Completion: Understanding Statistical Guarantees for Convex Relaxation via Nonconvex Optimization: Convex Relaxation Attains Near-Optimal Frobenius, Entrywise and Spectral Norm ErrorsResearch Paper

Motivation

Matrix completion asks for a low-rank matrix from a small random subset of its entries. It models collaborative filtering (recommendation systems), sensor-network localisation, and structure from motion. In practice the revealed entries are corrupted by noise, and the most widely used estimator is nuclear-norm regularized least squares: fit the observed entries in squared error while penalizing the sum of singular values. The estimator is a convex program, so it is solved reliably by proximal and singular-value-thresholding methods, and it needs no knowledge of the rank.

Its statistical accuracy was not understood. In the noiseless case, convex relaxation recovers the matrix exactly from nearly the information-theoretic minimum number of samples (Candès–Recht 2009, Candès–Tao 2010, Gross 2011). With noise, the available bounds for the plain convex program (Candès–Plan 2010) give ∥Zcvx−M⋆∥F≲σn3/2\|Z_{\rm cvx}-M^\star\|_F\lesssim\sigma n^{3/2}∥Zcvx​−M⋆∥F​≲σn3/2 under random noise. That can be a factor of order n2p\sqrt{n^2p}n2p​ above the oracle lower bound, and the numerical performance of the program is far better. Sharper rates were known only for modified estimators: Negahban–Wainwright 2012 add a spikiness constraint, Koltchinskii–Lounici–Tsybakov 2011 use a different estimator. In 2019, Chen, Chi, Fan, Ma and Yan (arXiv:1902.07698; SIAM J. Optim. 30(4), 2020, doi:10.1137/19M1290000) showed that the unmodified convex program attains near-optimal error in the Frobenius, entrywise and spectral norms simultaneously. Their argument goes through nonconvex gradient descent. This mission formalizes that theorem.

Setting

The unknown matrix is M⋆∈Rn×nM^\star\in\mathbb R^{n\times n}M⋆∈Rn×n of rank r≥1r\ge1r≥1, with singular value decomposition M⋆=U⋆Σ⋆V⋆⊤M^\star=U^\star\Sigma^\star V^{\star\top}M⋆=U⋆Σ⋆V⋆⊤. The columns of U⋆,V⋆∈Rn×rU^\star,V^\star\in\mathbb R^{n\times r}U⋆,V⋆∈Rn×r are orthonormal, and Σ⋆=diag(σ1⋆,…,σr⋆)\Sigma^\star=\mathrm{diag}(\sigma^\star_1,\dots,\sigma^\star_r)Σ⋆=diag(σ1⋆​,…,σr⋆​) with σmax⁡=max⁡kσk⋆\sigma_{\max}=\max_k\sigma^\star_kσmax​=maxk​σk⋆​, σmin⁡=min⁡kσk⋆>0\sigma_{\min}=\min_k\sigma^\star_k>0σmin​=mink​σk⋆​>0 and condition number κ=σmax⁡/σmin⁡\kappa=\sigma_{\max}/\sigma_{\min}κ=σmax​/σmin​. Write ∥A∥2,∞\|A\|_{2,\infty}∥A∥2,∞​ for the largest Euclidean norm of a row of AAA. M⋆M^\starM⋆ is μ\muμ-incoherent if ∥U⋆∥2,∞≤μr/n\|U^\star\|_{2,\infty}\le\sqrt{\mu r/n}∥U⋆∥2,∞​≤μr/n​ and ∥V⋆∥2,∞≤μr/n\|V^\star\|_{2,\infty}\le\sqrt{\mu r/n}∥V⋆∥2,∞​≤μr/n​ (Definition 1). Incoherence says that the energy of M⋆M^\starM⋆ is not concentrated on a few rows or columns.

Under Assumption 1, each index (i,j)(i,j)(i,j) enters the observed set Ω\OmegaΩ independently with probability ppp. One observes Mij=Mij⋆+EijM_{ij}=M^\star_{ij}+E_{ij}Mij​=Mij⋆​+Eij​ for (i,j)∈Ω(i,j)\in\Omega(i,j)∈Ω, where the EijE_{ij}Eij​ are i.i.d., zero-mean, and have sub-Gaussian norm ∥Eij∥ψ2=sup⁡q≥1q−1/2(E∣Eij∣q)1/q≤σ\|E_{ij}\|_{\psi_2}=\sup_{q\ge1}q^{-1/2}(\mathbb E|E_{ij}|^q)^{1/q}\le\sigma∥Eij​∥ψ2​​=supq≥1​q−1/2(E∣Eij​∣q)1/q≤σ. Let PΩ\mathcal P_\OmegaPΩ​ keep the entries indexed by Ω\OmegaΩ and zero the rest. The convex estimator is any minimizer ZcvxZ_{\rm cvx}Zcvx​ of

g(Z)=12∥PΩ(Z−M)∥F2+λ∥Z∥∗,λ=Cλσnp,(3)g(Z)=\tfrac12\|\mathcal P_\Omega(Z-M)\|_F^2+\lambda\|Z\|_*,\qquad\lambda=C_\lambda\sigma\sqrt{np},\qquad(3)g(Z)=21​∥PΩ​(Z−M)∥F2​+λ∥Z∥∗​,λ=Cλ​σnp​,(3)

where ∥Z∥∗\|Z\|_*∥Z∥∗​ is the nuclear norm, ∥⋅∥\|\cdot\|∥⋅∥ is the spectral norm and ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​ is the largest absolute entry.

Formalization targets

Goal: Theorem 2

Suppose n2p≥Cκ4μ2r2nlog⁡3nn^2p\ge C\kappa^4\mu^2r^2n\log^3nn2p≥Cκ4μ2r2nlog3n and σn/p≤c σmin⁡/κ4μrlog⁡n\sigma\sqrt{n/p}\le c\,\sigma_{\min}/\sqrt{\kappa^4\mu r\log n}σn/p​≤cσmin​/κ4μrlogn​. Then with probability 1−O(n−3)1-O(n^{-3})1−O(n−3), every minimizer of (3) satisfies

∥Zcvx−M⋆∥F≲κσσmin⁡np∥M⋆∥F,∥Zcvx−M⋆∥∞≲κ3μrσσmin⁡nlog⁡np∥M⋆∥∞,∥Zcvx−M⋆∥≲σσmin⁡np∥M⋆∥.\|Z_{\rm cvx}-M^\star\|_F\lesssim\kappa\tfrac{\sigma}{\sigma_{\min}}\sqrt{\tfrac np}\|M^\star\|_F,\quad\|Z_{\rm cvx}-M^\star\|_\infty\lesssim\sqrt{\kappa^3\mu r}\tfrac{\sigma}{\sigma_{\min}}\sqrt{\tfrac{n\log n}p}\|M^\star\|_\infty,\quad\|Z_{\rm cvx}-M^\star\|\lesssim\tfrac{\sigma}{\sigma_{\min}}\sqrt{\tfrac np}\|M^\star\|.∥Zcvx​−M⋆∥F​≲κσmin​σ​pn​​∥M⋆∥F​,∥Zcvx​−M⋆∥∞​≲κ3μr​σmin​σ​pnlogn​​∥M⋆∥∞​,∥Zcvx​−M⋆∥≲σmin​σ​pn​​∥M⋆∥.

Every best rank-rrr approximation Zcvx,rZ_{{\rm cvx},r}Zcvx,r​ is within n−3σσmin⁡n/p ∥M⋆∥n^{-3}\frac\sigma{\sigma_{\min}}\sqrt{n/p}\,\|M^\star\|n−3σmin​σ​n/p​∥M⋆∥ of ZcvxZ_{\rm cvx}Zcvx​ in Frobenius norm, and satisfies the same three bounds.

Milestones

  1. Deterministic layer: Lemma 20 (balancing an SVD factorization), Claim 3, Claim 2 and Lemma 2. Lemma 2 says that a point (X,Y)(X,Y)(X,Y) with ∥∇f(X,Y)∥F≤ccinjpκλpσmin⁡\|\nabla f(X,Y)\|_F\le c\frac{\sqrt{c_{\rm inj}p}}{\kappa}\frac\lambda p\sqrt{\sigma_{\min}}∥∇f(X,Y)∥F​≤cκcinj​p​​pλ​σmin​​ for the factored objective
f(X,Y)=12p∥PΩ(XY⊤−M)∥F2+λ2p(∥X∥F2+∥Y∥F2)f(X,Y)=\tfrac1{2p}\|\mathcal P_\Omega(XY^\top-M)\|_F^2+\tfrac\lambda{2p}(\|X\|_F^2+\|Y\|_F^2)f(X,Y)=2p1​∥PΩ​(XY⊤−M)∥F2​+2pλ​(∥X∥F2​+∥Y∥F2​)

satisfies ∥XY⊤−Zcvx∥F≤2304 κcinjσmin⁡∥∇f(X,Y)∥F\|XY^\top-Z_{\rm cvx}\|_F\le2304\,\frac{\kappa}{c_{\rm inj}\sqrt{\sigma_{\min}}}\|\nabla f(X,Y)\|_F∥XY⊤−Zcvx​∥F​≤2304cinj​σmin​​κ​∥∇f(X,Y)∥F​ under Conditions 1–2. 2. Probabilistic layer: Lemma 3 (Condition 1(a)), Lemma 19, Lemmas 7 and 8, and Lemma 4. Lemma 4 gives Conditions 1(b) and 2 uniformly over an ℓ2,∞\ell_{2,\infty}ℓ2,∞​ neighbourhood of the truth. 3. Algorithmic layer: Lemma 5, the error bounds and the small-gradient iterate of gradient descent started at the truth, and (31), its consequence for XtYt⊤−M⋆X^tY^{t\top}-M^\starXtYt⊤−M⋆.

Significance

The bounds of Theorem 2 match the minimax lower bounds up to logarithmic factors when rrr and κ\kappaκ are bounded. This holds in all three norms and for noise of any size below a threshold. The theorem also shows that the convex solution is nearly of rank rrr. Neither statement requires modifying the estimator, so practitioners running standard solvers get the guarantee as is. The entrywise bound (11b) shows an implicit regularization: the convex program spreads its error over all entries without being told to.

The theorem has a complete published proof. What this mission adds is a machine-checked version, which has value of its own here. The proof chains about twenty lemmas, including a leave-one-out analysis of gradient descent with polynomially many iterations. Its constants are hidden behind "≲\lesssim≲" at nearly every step. The formal development fixes the quantifier order of every such constant. It also records the hypotheses the proof uses without stating them, such as the independence of the sampling pattern from the noise. No part of this paper has been formalized before. The deterministic layer (Lemmas 20, 2, Claims 2–3) applies to any Burer–Monteiro factorization of a nuclear-norm problem, not only to this one.

Difficulty

The obvious approach is to analyse the convex program directly through a dual certificate, as in the noiseless theory. With noise there is no exact recovery, and the certificate approach loses a factor polynomial in nnn. The difficulty is to transfer statistical bounds from a point one can control, the nonconvex iterate, to a point one cannot construct, the convex minimizer. The two are compared through an approximate first-order condition. That comparison is useful only if injectivity and concentration hold uniformly over all factor pairs near the truth, because the iterates depend on Ω\OmegaΩ and on the noise. A fixed-tangent-space injectivity bound, the usual tool, does not suffice. The entrywise control of the iterates requires leave-one-out sequences, and those sequences make up most of the appendix.

Formalization scope

Matrices are Matrix (Fin n) (Fin n) ℝ and factors Matrix (Fin n) (Fin r) ℝ, using the published matrix_completion_basic, _svd and _tangent definitions (nuclear norm, SVD data, PΩ\mathcal P_\OmegaPΩ​, PT\mathcal P_TPT​, spectral, Frobenius and entrywise norms). M⋆M^\starM⋆ comes with an explicit SVD with r≥1r\ge1r≥1 positive singular values, so its rank is exactly rrr. Definition 1 is MatrixCompletion.A0. The sub-Gaussian bound is the moment form of [Ver12, Definition 5.7] above, not Mathlib's MGF form. The randomness lives on an arbitrary probability space. The sampling indicators and the noise entries are each mutually independent, and the two families are independent of each other. This last independence is an added hypothesis, which the paper's proofs use. "With probability 1−O(n−k)1-O(n^{-k})1−O(n−k)" is stated as an outer-measure bound Cfailn−kC_{\rm fail}n^{-k}Cfail​n−k on the failure event. Every unnamed constant ("≲\lesssim≲", "sufficiently large CCC", "sufficiently small ccc") is an existential placed before nnn and all data, together with an n0n_0n0​. Explicit constants of the paper are kept: the exponents −3-3−3 and −10-10−10, λ/8\lambda/8λ/8, 1/(32κ)1/(32\kappa)1/(32κ), 72κ72\kappa72κ, 8κ8\sqrt\kappa8κ​, t0=n18t_0=n^{18}t0​=n18, n−5n^{-5}n−5, the factors 333 in (31), the 1/n31/n^31/n3 in (12), and 2304=32⋅722304=32\cdot722304=32⋅72 in Lemma 2.

The goal keeps the randomness in the statement. A version with fixed Ω\OmegaΩ and EEE that assumes Conditions 1–2 or the conclusions of Lemma 5 would be Lemma 2 plus (31), not Theorem 2, and is not acceptable as a proof of the goal. The goal quantifies over every minimizer of (3) and every best rank-rrr approximation. Excluded: Theorem 1 (the r,κ=O(1)r,\kappa=O(1)r,κ=O(1) corollary), the noise condition of Remark 4, approximate minimizers (Remark 6), Lemmas 1 and 6, and the internal lemmas of the leave-one-out analysis (App. D), which solvers may add as supporting theorems. The development needs nuclear-norm subgradients, Weyl's inequality, matrix Bernstein and spectral-norm bounds for sparse random matrices. These are reusable well beyond this mission, and contributions of them are welcome. Theorem and equation numbers are those of the authors' preprint (Sep. 2019, arXiv:1902.07698) and may differ in the SIAM typesetting.

Selected references

  • Y. Chen, Y. Chi, J. Fan, C. Ma, Y. Yan, Noisy Matrix Completion: Understanding Statistical Guarantees for Convex Relaxation via Nonconvex Optimization, SIAM J. Optim. 30(4), 2020. https://doi.org/10.1137/19M1290000 (preprint: https://arxiv.org/abs/1902.07698)
  • E. J. Candès, B. Recht, Exact Matrix Completion via Convex Optimization, Found. Comput. Math. 9, 2009. https://doi.org/10.1007/s10208-009-9045-5
  • E. J. Candès, Y. Plan, Matrix Completion With Noise, Proc. IEEE 98(6), 2010. https://doi.org/10.1109/JPROC.2009.2035722
  • S. Negahban, M. J. Wainwright, Restricted strong convexity and weighted matrix completion: optimal bounds with noise, J. Mach. Learn. Res. 13, 2012. https://jmlr.org/papers/v13/negahban12a.html
  • V. Koltchinskii, K. Lounici, A. B. Tsybakov, Nuclear-norm penalization and optimal rates for noisy low-rank matrix completion, Ann. Statist. 39(5), 2011. https://doi.org/10.1214/11-AOS894
  • C. Ma, K. Wang, Y. Chi, Y. Chen, Implicit Regularization in Nonconvex Statistical Estimation, Found. Comput. Math. 20, 2020. https://doi.org/10.1007/s10208-019-09429-9
  • R. Vershynin, Introduction to the non-asymptotic analysis of random matrices, in Compressed Sensing: Theory and Applications, CUP, 2012. https://arxiv.org/abs/1011.3027
17 thms2 active usersReviewed
Information TheoryProbability·Captain: mikedeng1

Universality in Polytope Phase Transitions and Message Passing Algorithms 1: Polynomial AMP Iterates Have the Same Asymptotic Moments for All Sub-Gaussian Matrices with Equal Entry VariancesResearch Paper

Motivation

Approximate message passing (AMP) is a family of iterative algorithms driven by a large random matrix. It was introduced for compressed sensing by Donoho, Maleki and Montanari (PNAS 2009), and it is also used for low-rank matrix estimation, regression and spin-glass optimization. Its main appeal is that, for Gaussian random matrices, the empirical distribution of its iterates is tracked exactly in the large-dimensional limit by a scalar or low-dimensional recursion called state evolution. Bolthausen (CMP 2014) and Bayati and Montanari (IEEE Trans. Inf. Theory 2011) proved this for Gaussian matrices. Those proofs condition on the matrix through linear observations, and that conditioning argument works only for Gaussian entries.

In practice, and in the compressed-sensing phase transition that motivates the paper, the matrices are not Gaussian: Bernoulli, Rademacher and other sub-Gaussian ensembles are used. Bayati, Lelarge and Montanari (arXiv:1207.7321, Ann. Appl. Probab. 25(2), 2015) prove that the asymptotic behaviour of AMP with polynomial nonlinearities is universal: it depends on the law of the matrix entries only through their variances. This mission formalizes that universality theorem, Theorem 3 of the paper, together with the main steps of its proof.

Setting

Fix a dimension q≥1q \ge 1q≥1 and a degree bound d≥0d \ge 0d≥0. For each NNN, an AMP instance consists of three objects:

  • a symmetric matrix A∈RN×NA \in \mathbb R^{N\times N}A∈RN×N with Aii=0A_{ii} = 0Aii​=0;
  • polynomial maps fj(⋅ ;t):Rq→Rqf^j(\cdot\,; t):\mathbb R^q\to\mathbb R^qfj(⋅;t):Rq→Rq of degree at most ddd, one for each j∈[N]j\in[N]j∈[N] and each time t≥0t\ge 0t≥0;
  • an initial condition x0=(x10,…,xN0)x^0 = (x^0_1,\dots,x^0_N)x0=(x10​,…,xN0​) with xi0∈Rqx^0_i \in \mathbb R^qxi0​∈Rq.

The AMP orbit is

xit+1  =  ∑jAij fj(xjt;t)  −  ∑jAij2 ∂fj∂x(xjt;t) fi(xit−1;t−1),x^{t+1}_i \;=\; \sum_{j} A_{ij}\, f^j(x^t_j; t) \;-\; \sum_{j} A_{ij}^2\, \frac{\partial f^j}{\partial x}(x^t_j; t)\, f^i(x^{t-1}_i; t-1),xit+1​=j∑​Aij​fj(xjt​;t)−j∑​Aij2​∂x∂fj​(xjt​;t)fi(xit−1​;t−1),

where ∂fj/∂x\partial f^j/\partial x∂fj/∂x is the q×qq\times qq×q Jacobian. The second term, the memory or Onsager term, is absent at t=0t=0t=0. A sequence of random instances indexed by NNN is (C,d)(C,d)(C,d)-regular if it satisfies the following conditions:

  1. the entries AijA_{ij}Aij​, i<ji<ji<j, are independent and centered, and each is sub-Gaussian with scale factor C/NC/NC/N, that is, EeλAij≤eCλ2/(2N)\mathbb E e^{\lambda A_{ij}}\le e^{C\lambda^2/(2N)}EeλAij​≤eCλ2/(2N) for all real λ\lambdaλ;
  2. all coefficients of the polynomials are bounded by CCC;
  3. the matrix, the polynomials and the initial condition are mutually independent;
  4. ∑iexp⁡(∥xi0∥22/C)≤NC\sum_i \exp(\|x^0_i\|_2^2/C)\le NC∑i​exp(∥xi0​∥22​/C)≤NC.

The proof also uses an auxiliary message-passing iteration. It consists of messages zi→jt∈Rqz^t_{i\to j}\in\mathbb R^qzi→jt​∈Rq with zi→j0=xi0z^0_{i\to j}=x^0_izi→j0​=xi0​ and

zi→jt+1(r)=∑ℓ≠jAℓi frℓ(zℓ→it;t),zit+1(r)=∑ℓAℓi frℓ(zℓ→it;t).z^{t+1}_{i\to j}(r)=\sum_{\ell\neq j} A_{\ell i}\, f^\ell_r(z^t_{\ell\to i};t),\qquad z^{t+1}_{i}(r)=\sum_{\ell} A_{\ell i}\, f^\ell_r(z^t_{\ell\to i};t).zi→jt+1​(r)=ℓ=j∑​Aℓi​frℓ​(zℓ→it​;t),zit+1​(r)=ℓ∑​Aℓi​frℓ​(zℓ→it​;t).

Monomials are written xm=∏rx(r)m(r)x^m=\prod_r x(r)^{m(r)}xm=∏r​x(r)m(r) for m∈Nqm\in\mathbb N^qm∈Nq.

Formalization targets

Goal: Theorem 3 (p. 8)

Let (A(N),FN,x0,N)(A(N),\mathcal F_N,x^{0,N})(A(N),FN​,x0,N) and (A~(N),FN,x0,N)(\tilde A(N),\mathcal F_N,x^{0,N})(A~(N),FN​,x0,N) be two (C,d)(C,d)(C,d)-regular sequences. They share the polynomials and the initial condition, and EAij2=EA~ij2\mathbb E A_{ij}^2=\mathbb E\tilde A_{ij}^2EAij2​=EA~ij2​ for all i<ji<ji<j. Then for every ttt and every family of polynomials pN,i:Rq→Rp_{N,i}:\mathbb R^q\to\mathbb RpN,i​:Rq→R of degree at most ddd with coefficients bounded by BBB,

lim⁡N→∞1N∑i=1N{E pN,i(xit)−E pN,i(x~it)}=0.\lim_{N\to\infty}\frac1N\sum_{i=1}^N\Big\{\mathbb E\,p_{N,i}(x^t_i)-\mathbb E\,p_{N,i}(\tilde x^t_i)\Big\}=0 .N→∞lim​N1​i=1∑N​{EpN,i​(xit​)−EpN,i​(x~it​)}=0.

Milestones

  • Lemma 12 (p. 70): xs≤(s/e)sexx^s\le (s/e)^s e^xxs≤(s/e)sex for s,x>0s,x>0s,x>0.
  • (4.15) (p. 20): a sub-Gaussian variable with scale factor C/NC/NC/N satisfies E∣X∣s≤2Cs/2(s/e)s/2N−s/2\mathbb E|X|^s\le 2C^{s/2}(s/e)^{s/2}N^{-s/2}E∣X∣s≤2Cs/2(s/e)s/2N−s/2.
  • Proposition 1 (p. 16): ∣E(zit)m−E(z~it)m∣≤KN−1/2|\mathbb E(z^t_i)^m-\mathbb E(\tilde z^t_i)^m|\le KN^{-1/2}∣E(zit​)m−E(z~it​)m∣≤KN−1/2 for t≥1t\ge1t≥1.
  • Lemma 2, uniform bounds (pp. 22–23): ∣Ezit(r)m∣≤K|\mathbb E z^t_i(r)^m|\le K∣Ezit​(r)m∣≤K and ∣Ezi→jt(r)m∣≤K|\mathbb E z^t_{i\to j}(r)^m|\le K∣Ezi→jt​(r)m∣≤K.
  • Proposition 3 (p. 17), averaged over coordinates: 1N∑i∣E(xit)m−E(zit)m∣≤KN−1/2\frac1N\sum_i|\mathbb E(x^t_i)^m-\mathbb E(z^t_i)^m|\le KN^{-1/2}N1​∑i​∣E(xit​)m−E(zit​)m∣≤KN−1/2 for t≥1t\ge1t≥1. The page states the bound for each iii; that form fails when one coordinate of x0,Nx^{0,N}x0,N grows like log⁡N\sqrt{\log N}logN​, which Definition 4(3) permits, and the averaged form is what Theorem 3 needs.

In each milestone KKK depends only on C,d,q,t,mC,d,q,t,mC,d,q,t,m, as Note 2 of the paper specifies.

Significance

Theorem 3 lets results proved for Gaussian matrices be transferred to every sub-Gaussian ensemble with the same variance profile. In the paper, it is the first link of a chain:

  • Theorem 3 gives state evolution for general matrices (Theorem 4, the second mission of this series);
  • state evolution, together with an analysis of AMP as a solver of ℓ1\ell_1ℓ1​ minimization, gives the universality of the Donoho–Tanner phase transition for random projections of the cross-polytope (Theorem 2, the third mission).

The universality of the weak-neighborliness threshold for non-Gaussian matrices, observed numerically by Donoho and Tanner (Phil. Trans. R. Soc. A 2009), is a consequence of this chain.

The result has been proved since 2012. No machine-checked proof of it, or of any AMP state-evolution statement, is known to exist. The mission asks for a formalization of the published proof, or of any other argument. Two pieces of the proof are useful elsewhere: the absolute-moment bound for sub-Gaussian variables and the moment comparison of the message-passing iteration.

Difficulty

The first idea is a Lindeberg-type swap: replace the entries of AAA by those of A~\tilde AA~ one at a time and bound each change. This does not work directly. Every iterate xitx^t_ixit​ depends on all N(N−1)/2N(N-1)/2N(N−1)/2 entries through ttt nested polynomial layers. The memory term also couples consecutive iterates through the squares Aij2A_{ij}^2Aij2​. A single swap therefore changes every coordinate of every later iterate, and the per-swap errors have to be summed over Θ(N2)\Theta(N^2)Θ(N2) swaps with a total error of o(1)o(1)o(1).

Two features of the statement make it delicate. Only second moments of the entries are matched, so every contribution of higher moments of the entries must be shown to vanish in the limit. In addition, the AMP orbit is not itself a message-passing iteration: its moments match those of ztz^tzt (Proposition 3) only because of the memory term, and without that term they do not. A formal proof also has to establish finiteness of all the moments involved, which the paper takes for granted.

Formalization scope

Vectors in Rq\mathbb R^qRq are Fin q → ℝ, and indices are 0-based. A polynomial is given by its coefficient vector over the exponent vectors of total degree at most ddd, as in (4.10) of the paper. This keeps random polynomials in a measurable space. The Jacobian is the explicit sum of formal partial derivatives. A sorry-free sanity file checks it against the analytic derivative on an example and checks the memory term on a small instance.

The orbit is computed by recursion on (xt,xt−1)(x^t,x^{t-1})(xt,xt−1), with no memory term at t=0t=0t=0. The memory term uses Aij2A_{ij}^2Aij2​ itself, not its expectation 1/N1/N1/N. All random objects live on one probability space. The two sequences of Theorem 3 share one coefficient process and one initial condition.

Three readings of the printed Definition 4 are disclosed:

  • sub-Gaussianity is required for all real λ\lambdaλ (Mathlib's HasSubgaussianMGF), not only for λ>0\lambda > 0λ>0;
  • the scale factor is C/NC/NC/N, as the proof uses. The printed bracket (Cλ)2/(2N2)(C\lambda)^2/(2N^2)(Cλ)2/(2N2) would rule out every ensemble with variance 1/N1/N1/N once N>C2N > C^2N>C2, which would make the theorem vacuous;
  • the initial-condition bound holds almost surely for every NNN, not "with probability converging to one".

Every expectation appearing in a target is also asserted to be finite. Without that, a bound or a limit could hold only because Lean assigns the value 000 to the integral of a non-integrable function. Squared Euclidean norms are written as sums of squares, never as the sup norm that Mathlib puts on Fin q → ℝ. The deterministic identities of the tree expansion (Lemma 1, Lemma 3) and the first claim of Lemma 2 are not posed, because they need the labelled-tree families of Definition 6. Contributions of that tree machinery are welcome. Moment bounds for sub-Gaussian variables and polynomial moment estimates for sums of independent variables are reusable well beyond this mission.

Selected references

  • M. Bayati, M. Lelarge, A. Montanari, Universality in polytope phase transitions and message passing algorithms, Ann. Appl. Probab. 25(2):753–822, 2015. arXiv:1207.7321v2, DOI
  • D. L. Donoho, A. Maleki, A. Montanari, Message-passing algorithms for compressed sensing, PNAS 106(45):18914–18919, 2009. DOI
  • M. Bayati, A. Montanari, The dynamics of message passing on dense graphs, with applications to compressed sensing, IEEE Trans. Inf. Theory 57(2):764–785, 2011. DOI
  • E. Bolthausen, An iterative construction of solutions of the TAP equations for the Sherrington–Kirkpatrick model, Comm. Math. Phys. 325:333–366, 2014. DOI
  • D. L. Donoho, J. Tanner, Observed universality of phase transitions in high-dimensional geometry, Phil. Trans. R. Soc. A 367:4273–4293, 2009. DOI
9 thms2 active usersReviewed
Linear algebraProbabilityStatistics·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices IV: The Matrix Bennett and Bernstein Inequalities for Independent Zero-Mean Random Matrices with Bounded Largest EigenvalueResearch Paper

Motivation

The scalar Bernstein and Bennett inequalities bound the upper tail of a sum of independent, zero-mean random variables that are bounded above: the tail is governed by the total variance at moderate deviations and by the uniform bound in the far tail. Many questions in randomized numerical linear algebra, matrix completion, covariance estimation, graph sparsification and statistical learning reduce to the same question for a sum of independent random matrices, where the quantity of interest is the largest eigenvalue or the spectral norm of the sum rather than a scalar.

Ahlswede and Winter (2002) introduced a matrix Laplace transform method based on the Golden–Thompson inequality. Oliveira (2010) and Gross (2011) proved matrix Bernstein-type bounds with this method. Tropp (arXiv:1004.4389, Found. Comput. Math. 12 (2012)) replaced the Golden–Thompson step with Lieb's concavity theorem, obtaining a master tail bound for independent sums (Theorem 3.6) from which matrix Bennett and Bernstein inequalities follow with the variance parameter ∥∑kEXk2∥\|\sum_k \mathbb E X_k^2\|∥∑k​EXk2​∥, the natural analogue of the scalar variance. This mission formalizes §6 of that paper.

Timeline:

  • 1924–1962, Bernstein and Bennett: scalar inequalities for bounded and subexponential sums.
  • 2002, Ahlswede–Winter: the matrix Laplace transform method, via Golden–Thompson.
  • 2010, Oliveira; Gross: matrix Bernstein-type bounds by the Ahlswede–Winter method.
  • 2010–2012, Tropp: master tail bound via Lieb's theorem; matrix Bennett and Bernstein inequalities (Theorems 6.1, 6.2) with variance parameter ∥∑kEXk2∥\|\sum_k\mathbb E X_k^2\|∥∑k​EXk2​∥.

Setting

All matrices are d×dd\times dd×d complex matrices with d≥1d\ge 1d≥1. For a self-adjoint (Hermitian) matrix AAA, λmax⁡(A)\lambda_{\max}(A)λmax​(A) is its largest eigenvalue and ∥A∥\|A\|∥A∥ its spectral norm. The semidefinite order A≼BA\preccurlyeq BA≼B means that B−AB-AB−A is positive semidefinite. Functions of a self-adjoint matrix are defined spectrally: if A=QΛQ∗A=Q\Lambda Q^*A=QΛQ∗, then f(A)=Qf(Λ)Q∗f(A)=Qf(\Lambda)Q^*f(A)=Qf(Λ)Q∗; this gives the matrix exponential eAe^AeA and, on positive-definite matrices, the matrix logarithm log⁡A\log AlogA. The trace is tr⁡\operatorname{tr}tr.

A random matrix is a measurable map X:Ω→Cd×dX:\Omega\to\mathbb C^{d\times d}X:Ω→Cd×d on a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P); its expectation EX\mathbb E XEX is taken entrywise. A finite sequence X1,…,XnX_1,\dots,X_nX1​,…,Xn​ of random self-adjoint matrices is independent if the maps are mutually independent.

The setting of the goal: X1,…,XnX_1,\dots,X_nX1​,…,Xn​ are independent random self-adjoint matrices with

EXk=0andλmax⁡(Xk)≤R almost surely,\mathbb E X_k=0\qquad\text{and}\qquad \lambda_{\max}(X_k)\le R\ \text{almost surely},EXk​=0andλmax​(Xk​)≤R almost surely,

and the total variance is σ2:=∥∑kE(Xk2)∥\sigma^2:=\big\|\sum_k \mathbb E(X_k^2)\big\|σ2:=​∑k​E(Xk2​)​. Bennett's function is h(u):=(1+u)log⁡(1+u)−uh(u):=(1+u)\log(1+u)-uh(u):=(1+u)log(1+u)−u for u≥0u\ge0u≥0.

Formalization targets

Goal: Theorem 6.1 (matrix Bernstein, bounded case)

For every t≥0t\ge0t≥0, the following chain holds:

P{λmax⁡(∑kXk)≥t}≤d⋅exp⁡(−σ2R2 h(Rtσ2))≤d⋅exp⁡(−t2/2σ2+Rt/3),\mathbb P\Big\{\lambda_{\max}\Big(\sum_k X_k\Big)\ge t\Big\}\le d\cdot\exp\Big(-\frac{\sigma^2}{R^2}\,h\Big(\frac{Rt}{\sigma^2}\Big)\Big)\le d\cdot\exp\Big(\frac{-t^2/2}{\sigma^2+Rt/3}\Big),P{λmax​(k∑​Xk​)≥t}≤d⋅exp(−R2σ2​h(σ2Rt​))≤d⋅exp(σ2+Rt/3−t2/2​),

and the last term is at most d e−3t2/8σ2d\,e^{-3t^2/8\sigma^2}de−3t2/8σ2 for t≤σ2/Rt\le\sigma^2/Rt≤σ2/R and at most d e−3t/8Rd\,e^{-3t/8R}de−3t/8R for t≥σ2/Rt\ge\sigma^2/Rt≥σ2/R. The first inequality is the matrix Bennett inequality, the second the matrix Bernstein inequality, and the case split the split Bernstein inequality.

Milestones, in attack order

  1. Theorem 3.6, the master tail bound P{λmax⁡(∑kXk)≥t}≤e−θttr⁡exp⁡(∑klog⁡EeθXk)\mathbb P\{\lambda_{\max}(\sum_k X_k)\ge t\}\le e^{-\theta t}\operatorname{tr}\exp(\sum_k\log\mathbb E e^{\theta X_k})P{λmax​(∑k​Xk​)≥t}≤e−θttrexp(∑k​logEeθXk​) for θ>0\theta>0θ>0.
  2. Corollary 3.7: a semidefinite bound EeθXk≼eg(θ)Ak\mathbb E e^{\theta X_k}\preccurlyeq e^{g(\theta)A_k}EeθXk​≼eg(θ)Ak​ gives P{λmax⁡(∑kXk)≥t}≤d e−θt+g(θ)λmax⁡(∑kAk)\mathbb P\{\lambda_{\max}(\sum_k X_k)\ge t\}\le d\,e^{-\theta t+g(\theta)\lambda_{\max}(\sum_k A_k)}P{λmax​(∑k​Xk​)≥t}≤de−θt+g(θ)λmax​(∑k​Ak​).
  3. Lemma 6.7: if EX=0\mathbb E X=0EX=0 and λmax⁡(X)≤1\lambda_{\max}(X)\le1λmax​(X)≤1, then EeθX≼exp⁡((eθ−θ−1) EX2)\mathbb E e^{\theta X}\preccurlyeq\exp\big((e^\theta-\theta-1)\,\mathbb E X^2\big)EeθX≼exp((eθ−θ−1)EX2) for θ>0\theta>0θ>0.
  4. Theorem 6.1(i), the matrix Bennett inequality on its own.
  5. The numerical bound h(u)≥u2/21+u/3h(u)\ge\dfrac{u^2/2}{1+u/3}h(u)≥1+u/3u2/2​ for u≥0u\ge0u≥0, from the proof of Theorem 6.1.

Further items

Lemma 6.8 (the matrix mgf bound EeθX≼exp⁡(θ22(1−θ)A2)\mathbb E e^{\theta X}\preccurlyeq\exp(\frac{\theta^2}{2(1-\theta)}A^2)EeθX≼exp(2(1−θ)θ2​A2) under EXp≼p!2A2\mathbb E X^p\preccurlyeq\frac{p!}{2}A^2EXp≼2p!​A2) and Theorem 6.2 (matrix Bernstein, subexponential case: P{λmax⁡(∑kXk)≥t}≤dexp⁡(−t2/2σ2+Rt)\mathbb P\{\lambda_{\max}(\sum_k X_k)\ge t\}\le d\exp(\frac{-t^2/2}{\sigma^2+Rt})P{λmax​(∑k​Xk​)≥t}≤dexp(σ2+Rt−t2/2​), split as d e−t2/4σ2d\,e^{-t^2/4\sigma^2}de−t2/4σ2 and d e−t/4Rd\,e^{-t/4R}de−t/4R) are included as further theorems.

Significance

Matrix Bernstein is the most used inequality of the paper: it bounds the spectral norm of a sum of independent bounded random matrices with only a logarithmic dimensional factor, and it is the standard tool behind sampling bounds for matrix completion, randomized low-rank approximation, spectral sparsification, covariance estimation and the analysis of random features. Theorem 6.1 assumes only an upper bound on the largest eigenvalue of each summand, so it applies to summands with unbounded smallest eigenvalues; applied to {Xk}\{X_k\}{Xk​} and {−Xk}\{-X_k\}{−Xk​} separately it controls both tails.

The results are proved in the paper. As far as the local catalog shows, no machine-checked proof of the matrix Bennett or Bernstein inequality for complex Hermitian matrices exists; the platform has a matrix Bernstein statement for real symmetric matrices in a different form (Wainwright, Theorem 6.17), still open, and scalar Bennett and Bernstein inequalities. Formalizing Theorem 6.1 produces a reusable matrix concentration inequality together with its two ingredients, the matrix mgf bound of Lemma 6.7 and the scalar inequality relating Bennett's and Bernstein's exponents.

Difficulty

The scalar argument multiplies moment generating functions of independent summands. For matrices, eA+B≠eAeBe^{A+B}\ne e^Ae^BeA+B=eAeB unless AAA and BBB commute, so E tr⁡eθ∑kXk\mathbb E\,\operatorname{tr} e^{\theta\sum_k X_k}Etreθ∑k​Xk​ does not factor; the master bound of Theorem 3.6 rests on Lieb's concavity theorem for A↦tr⁡exp⁡(H+log⁡A)A\mapsto\operatorname{tr}\exp(H+\log A)A↦trexp(H+logA), which is not in Mathlib. The mgf bound of Lemma 6.7 needs a semidefinite comparison between functions of a random matrix, the transfer rule f≤gf\le gf≤g on the spectrum ⇒f(A)≼g(A)\Rightarrow f(A)\preccurlyeq g(A)⇒f(A)≼g(A), and the operator monotonicity of the logarithm. The remaining steps (optimizing over θ\thetaθ, the inequality between hhh and the Bernstein exponent) are real analysis.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ with [NeZero d]; λmax⁡\lambda_{\max}λmax​ is the supremum of the real spectrum; ∥⋅∥\|\cdot\|∥⋅∥ is the operator norm on ℓ2d\ell_2^dℓ2d​; eAe^AeA and log⁡A\log AlogA are Mathlib's continuous functional calculus cfc; the semidefinite order is Mathlib's MatrixOrder; expectation is entrywise. A random matrix is a measurable map, each XkX_kXk​ is Hermitian at every ω\omegaω, independence is iIndepFun, and the measure is a probability measure. The bound λmax⁡(Xk)≤R\lambda_{\max}(X_k)\le Rλmax​(Xk​)≤R is assumed almost surely; no lower bound on the eigenvalues is assumed. The paper's standing regularity (§2.2) is made explicit as integrability of the entries of XkX_kXk​ and Xk2X_k^2Xk2​ (and of eθXke^{\theta X_k}eθXk​ where its expectation is taken). The infimum over θ>0\theta>0θ>0 in Theorem 3.6 and Corollary 3.7 is stated for every admissible θ>0\theta>0θ>0.

The printed formulas divide by RRR and σ2\sigma^2σ2, so 0<R0<R0<R and 0<σ20<\sigma^20<σ2 are hypotheses of Theorems 6.1 and 6.2; with Lean's convention x/0=0x/0=0x/0=0, the case σ2=0\sigma^2=0σ2=0 would turn the Bennett bound into the trivial value ddd, so the statement is not allowed to degenerate there. The chain is a conjunction of the probability bound and the inequalities between consecutive bounds, so the weaker reading "the probability is below each bound" does not satisfy it.

A complete development needs the matrix Laplace transform method, Lieb's theorem (or a substitute), operator monotonicity of the logarithm, the transfer rule for the functional calculus, and the scalar inequality h(u)≥(u2/2)/(1+u/3)h(u)\ge(u^2/2)/(1+u/3)h(u)≥(u2/2)/(1+u/3). The first four are reusable for every matrix concentration inequality of this paper and beyond. Contributions to any milestone are welcome.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, arXiv:1004.4389v7, 2011; Found. Comput. Math. 12 (2012) 389–434. https://arxiv.org/abs/1004.4389, https://doi.org/10.1007/s10208-011-9099-z
  • R. Ahlswede and A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48 (2002) 569–579. https://doi.org/10.1109/18.985947
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
  • D. Gross, Recovering low-rank matrices from few coefficients in any basis, IEEE Trans. Inform. Theory 57 (2011) 1548–1566. https://arxiv.org/abs/0910.1879
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
  • G. Lugosi, Concentration-of-measure inequalities, lecture notes, 2009 (Theorems 5 and 6, scalar Bennett and Bernstein). https://www.econ.upf.edu/~lugosi/anu.pdf
9 thms2 active usersReviewed
Linear algebraProbability·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices II: Matrix Gaussian and Rademacher Series Have Subgaussian Tails with Variance Parameter ‖Σ A_k²‖Research Paper

Motivation

A matrix Gaussian series ∑kγkAk\sum_k \gamma_k A_k∑k​γk​Ak​, a sum of fixed self-adjoint matrices each multiplied by an independent standard normal variable, is the simplest sum of independent random matrices. It already appears in the analysis of random designs, in compressed sensing, in randomized numerical linear algebra and in quantum information, wherever one needs to know how large the spectrum of a random linear combination of matrices can be. Its Rademacher analogue ∑kεkAk\sum_k \varepsilon_k A_k∑k​εk​Ak​, with random signs, plays the same role in symmetrization arguments.

For real coefficients aka_kak​ the answer is classical: ∑kγkak\sum_k \gamma_k a_k∑k​γk​ak​ is normal with variance ∑kak2\sum_k a_k^2∑k​ak2​, so its upper tail is at most e−t2/2σ2e^{-t^2/2\sigma^2}e−t2/2σ2. Tropp's paper (arXiv:1004.4389v7) shows that the same bound holds for the largest eigenvalue of a matrix series, with an explicit dimensional factor and with the variance parameter ∥∑kAk2∥\|\sum_k A_k^2\|∥∑k​Ak2​∥.

Timeline. Noncommutative Khintchine inequalities (Lust-Piquard 1986; Lust-Piquard and Pisier 1991) control the moments of matrix Rademacher and Gaussian series and imply tail bounds of this type. Ahlswede and Winter (2002, arXiv:quant-ph/0012127) introduced the matrix Laplace transform method, whose bounds depend on the sum of the norms ∑k∥Ak2∥\sum_k\|A_k^2\|∑k​∥Ak2​∥. Oliveira (2010, arXiv:1004.3821) obtained bounds of the same form as Theorem 4.1. Tropp (2012) derived the result from a master inequality built on Lieb's concavity theorem (1973), which produces the norm of the sum, ∥∑kAk2∥\|\sum_k A_k^2\|∥∑k​Ak2​∥, as variance parameter. The paper itself notes that Theorem 4.1 and Corollary 4.2 are not new results; the contribution is the route through the master bound.

Setting

Fix a dimension d≥1d\ge1d≥1. Matrices are d×dd\times dd×d complex arrays; a matrix is self-adjoint if it equals its conjugate transpose. For a self-adjoint AAA, λmax⁡(A)\lambda_{\max}(A)λmax​(A) is its largest eigenvalue, and ∥A∥\|A\|∥A∥ is the spectral norm, the operator norm on Cd\mathbb C^dCd with the Euclidean norm. Functions of a self-adjoint matrix are defined through its eigen-decomposition: eAe^AeA, log⁡A\log AlogA (for positive-definite AAA), cosh⁡A\cosh AcoshA. The semidefinite order A≼HA\preccurlyeq HA≼H means that H−AH-AH−A is positive semidefinite.

A random matrix is a measurable map from a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) into the d×dd\times dd×d complex matrices; its expectation EX\mathbb E XEX is taken entry by entry. A Rademacher variable takes the values ±1\pm1±1 with probability 1/21/21/2 each; a standard normal variable has law N(0,1)N(0,1)N(0,1).

The data of the mission are fixed self-adjoint matrices A1,…,AnA_1,\dots,A_nA1​,…,An​ and independent scalar variables ξ1,…,ξn\xi_1,\dots,\xi_nξ1​,…,ξn​, all standard normal or all Rademacher. The variance parameter is

σ2:=∥∑kAk2∥.\sigma^2 := \Big\|\sum_k A_k^2\Big\|.σ2:=​k∑​Ak2​​.

Formalization targets

Goal: Theorem 4.1 (p. 14)

For all t≥0t\ge0t≥0,

P{λmax⁡(∑kξkAk)≥t}≤d e−t2/2σ2,P{∥∑kξkAk∥≥t}≤2d e−t2/2σ2.\mathbb P\Big\{\lambda_{\max}\Big(\sum_k\xi_kA_k\Big)\ge t\Big\}\le d\,e^{-t^2/2\sigma^2},\qquad \mathbb P\Big\{\Big\|\sum_k\xi_kA_k\Big\|\ge t\Big\}\le 2d\,e^{-t^2/2\sigma^2}.P{λmax​(k∑​ξk​Ak​)≥t}≤de−t2/2σ2,P{​k∑​ξk​Ak​​≥t}≤2de−t2/2σ2.

Milestones

  1. Theorem 3.6 (master tail bound, p. 12): for independent random self-adjoint XkX_kXk​ and every ttt,
P{λmax⁡(∑kXk)≥t}≤inf⁡θ>0e−θttr⁡exp⁡(∑klog⁡EeθXk).\mathbb P\Big\{\lambda_{\max}\Big(\sum_kX_k\Big)\ge t\Big\}\le\inf_{\theta>0}e^{-\theta t}\operatorname{tr}\exp\Big(\sum_k\log\mathbb Ee^{\theta X_k}\Big).P{λmax​(k∑​Xk​)≥t}≤θ>0inf​e−θttrexp(k∑​logEeθXk​).
  1. Corollary 3.7 (p. 12): if EeθXk≼eg(θ)Ak\mathbb Ee^{\theta X_k}\preccurlyeq e^{g(\theta)A_k}EeθXk​≼eg(θ)Ak​ with g≥0g\ge0g≥0, then the tail is at most dinf⁡θ>0e−θt+g(θ)ρd\inf_{\theta>0}e^{-\theta t+g(\theta)\rho}dinfθ>0​e−θt+g(θ)ρ with ρ=λmax⁡(∑kAk)\rho=\lambda_{\max}(\sum_kA_k)ρ=λmax​(∑k​Ak​).
  2. Display (2.4) (p. 8): cosh⁡(A)≼eA2/2\cosh(A)\preccurlyeq e^{A^2/2}cosh(A)≼eA2/2 for every self-adjoint AAA.
  3. Lemma 4.3 (p. 15): EeεθA≼eθ2A2/2\mathbb Ee^{\varepsilon\theta A}\preccurlyeq e^{\theta^2A^2/2}EeεθA≼eθ2A2/2 for Rademacher ε\varepsilonε and EeγθA=eθ2A2/2\mathbb Ee^{\gamma\theta A}=e^{\theta^2A^2/2}EeγθA=eθ2A2/2 for standard normal γ\gammaγ.

Further item: Corollary 4.2 (p. 15)

For fixed d1×d2d_1\times d_2d1​×d2​ matrices BkB_kBk​ and σ2=max⁡{∥∑kBkBk∗∥,∥∑kBk∗Bk∥}\sigma^2=\max\{\|\sum_kB_kB_k^*\|,\|\sum_kB_k^*B_k\|\}σ2=max{∥∑k​Bk​Bk∗​∥,∥∑k​Bk∗​Bk​∥},

P{∥∑kξkBk∥≥t}≤(d1+d2) e−t2/2σ2.\mathbb P\Big\{\Big\|\sum_k\xi_kB_k\Big\|\ge t\Big\}\le(d_1+d_2)\,e^{-t^2/2\sigma^2}.P{​k∑​ξk​Bk​​≥t}≤(d1​+d2​)e−t2/2σ2.

Significance

The result. Theorem 4.1 is the template for every inequality in the paper: a scalar tail bound carried over to matrices at the cost of a factor ddd, with a variance parameter that is the norm of a sum rather than a sum of norms. The difference matters: ∑k∥Ak2∥\sum_k\|A_k^2\|∑k​∥Ak2​∥ can exceed ∥∑kAk2∥\|\sum_kA_k^2\|∥∑k​Ak2​∥ by a factor of ddd, and §4 of the paper shows that both the variance parameter and the dimensional factor in (4.3) are needed in general. Corollary 4.2 transfers the bound to the largest singular value of a rectangular series, which covers Gaussian matrices with nonuniform variances (§4.3).

Formalizing it. The theorem is proved in the paper; the work here is to formalize that proof. The milestones are reusable beyond this mission: Theorem 3.6 and Corollary 3.7 are the common entry point of the Chernoff, Bernstein and Azuma missions of this series, and the Rademacher half of Lemma 4.3 is used again in the matrix Azuma mission. No machine-checked proof of these matrix inequalities was found in Mathlib or on the platform when this mission was drafted.

Difficulty

The scalar argument bounds Eeθ∑kXk\mathbb E e^{\theta\sum_k X_k}Eeθ∑k​Xk​ by the product of the individual mgfs, using ea+b=eaebe^{a+b}=e^ae^bea+b=eaeb. For matrices this identity fails when the summands do not commute, and the trace inequality that replaces it for two matrices (Golden–Thompson) has no analogue for three or more. Controlling the trace mgf of a sum of many noncommuting independent matrices therefore requires a genuinely matrix-analytic input with no scalar counterpart; the naive product bound is not available. A second difficulty is infrastructural: matrix functions, the semidefinite order and expectations of random matrices must be combined in a single setting.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ with [NeZero d]; self-adjointness is IsHermitian; eAe^AeA, log⁡A\log AlogA, cosh⁡A\cosh AcoshA are Mathlib's continuous functional calculus cfc; ≼\preccurlyeq≼ is Mathlib's Loewner order under MatrixOrder; λmax⁡\lambda_{\max}λmax​ is the supremum of the real spectrum; ∥⋅∥\|\cdot\|∥⋅∥ is the operator norm on ℓ2\ell_2ℓ2​. Expectation is entrywise, and the paper's standing regularity assumption is made explicit as entrywise integrability of every matrix whose expectation is taken. The infimum over θ>0\theta>0θ>0 is stated pointwise: the bound is asserted for every θ>0\theta>0θ>0 at which the mgfs exist, which is equivalent to the infimum form. Independence is iIndepFun of the scalar variables, and "Gaussian or Rademacher" is the disjunction of two hypotheses, never a mixture of laws.

The variance parameter is the norm of the sum ∥∑kAk2∥\|\sum_kA_k^2\|∥∑k​Ak2​∥; a formalization with ∑k∥Ak2∥\sum_k\|A_k^2\|∑k​∥Ak2​∥, with a constant different from 1/21/21/2, or with the dimensional factor omitted is a different theorem. At σ2=0\sigma^2=0σ2=0, Lean's division by zero makes the bound the trivial ddd; this is the only degenerate case and it is valid.

The development needs: the spectral calculus for Hermitian matrices, monotonicity of the trace exponential, operator monotonicity of the matrix logarithm, Lieb's theorem, and moments of the Gaussian. These are reusable well beyond this paper; proofs of the milestones, of supporting matrix-analysis lemmas, and alternative routes (for instance through noncommutative Khintchine inequalities) are all welcome.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, Found. Comput. Math. 12 (2012) 389–434; cited from arXiv:1004.4389v7. https://arxiv.org/abs/1004.4389, https://doi.org/10.1007/s10208-011-9099-z
  • R. Ahlswede and A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48 (2002) 569–579. https://arxiv.org/abs/quant-ph/0012127
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
  • F. Lust-Piquard and G. Pisier, Non commutative Khintchine and Paley inequalities, Ark. Mat. 29 (1991) 241–260. https://doi.org/10.1007/BF02384340
8 thms2 active usersReviewed
Linear algebraProbability·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices I: The Master Tail Bound — the Largest Eigenvalue of an Independent Sum Is Controlled by the Sum of the Matrix Cumulant Generating FunctionsResearch Paper

Motivation

Sums of independent random matrices appear wherever a large matrix is built from random pieces: sample covariance matrices in statistics, random sparsification and sampling in numerical linear algebra, random graphs and their Laplacians, and compressed sensing. The basic question is how far the largest eigenvalue of such a sum can stray above its typical value. For sums of independent real random variables the answer is given by the classical inequalities of Chernoff, Hoeffding and Bernstein, all derived by the Laplace transform method: bound the tail by the moment generating function, and use independence to factor the moment generating function of the sum.

Ahlswede and Winter (2002) showed that a matrix analogue of the Laplace transform method exists, and Oliveira (2010) refined the starting inequality. Tropp's paper (arXiv:1004.4389) replaced the Ahlswede–Winter decoupling step by a consequence of Lieb's concavity theorem (Lieb 1973) and obtained a single master tail bound from which matrix versions of the Gaussian-series, Chernoff, Bernstein and Azuma inequalities follow with sharp variance parameters. This mission formalizes that master bound, the first of five missions covering the paper.

Timeline:

  • 1973: Lieb proves concavity of A↦tr⁡exp⁡(H+log⁡A)A\mapsto \operatorname{tr}\exp(H+\log A)A↦trexp(H+logA) on positive-definite matrices; Epstein gives a second proof (Epstein 1973).
  • 2002: Ahlswede and Winter introduce the matrix Laplace transform method, decoupling summands with the Golden–Thompson inequality.
  • 2010: Oliveira's variant of the matrix Laplace transform bound.
  • 2010–2012: Tropp derives the master bound for independent sums from Lieb's theorem (journal version: Found. Comput. Math. 12 (2012)); in 2011 he also derives Lieb's theorem from the joint convexity of quantum relative entropy (arXiv:1101.1070).

Setting

All matrices are d×dd\times dd×d arrays of complex numbers with d≥1d\ge1d≥1. A matrix AAA is self-adjoint (Hermitian) when A=A∗A=A^*A=A∗; it then has real eigenvalues, and λmax⁡(A)\lambda_{\max}(A)λmax​(A) denotes the largest one. For a function f:R→Rf:\mathbb R\to\mathbb Rf:R→R and a self-adjoint A=QΛQ∗A=Q\Lambda Q^*A=QΛQ∗ with QQQ unitary and Λ\LambdaΛ diagonal, f(A):=Qf(Λ)Q∗f(A):=Qf(\Lambda)Q^*f(A):=Qf(Λ)Q∗. This defines the matrix exponential eAe^{A}eA of every self-adjoint matrix and the matrix logarithm log⁡A\log AlogA of every positive-definite matrix, with log⁡(eA)=A\log(e^A)=Alog(eA)=A. The trace exponential is A↦tr⁡eAA\mapsto\operatorname{tr}e^{A}A↦treA.

A random self-adjoint matrix is a measurable map XXX from a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P) to the self-adjoint matrices. Its expectation EX\mathbb E XEX is the matrix of the expectations of its entries. A finite sequence X1,…,XnX_1,\dots,X_nX1​,…,Xn​ is independent when the maps are jointly independent. The matrix moment generating function and matrix cumulant generating function of XXX are

MX(θ):=E eθX,ΞX(θ):=log⁡E eθX,θ∈R,M_X(\theta):=\mathbb E\,e^{\theta X},\qquad \Xi_X(\theta):=\log\mathbb E\,e^{\theta X},\qquad\theta\in\mathbb R,MX​(θ):=EeθX,ΞX​(θ):=logEeθX,θ∈R,

which may fail to exist for some θ\thetaθ. In the Lean development these objects are lambdaMax, mexp, mlog, trExp and mean in the namespace MatrixTail.Master.

Formalization targets

Goal: the master tail bound (Theorem 3.6)

For independent random self-adjoint matrices X1,…,XnX_1,\dots,X_nX1​,…,Xn​ and every t∈Rt\in\mathbb Rt∈R,

P{λmax⁡(∑kXk)≥t}≤inf⁡θ>0{e−θt⋅tr⁡exp⁡(∑klog⁡E eθXk)}.\mathbb P\Bigl\{\lambda_{\max}\Bigl(\sum_k X_k\Bigr)\ge t\Bigr\}\le\inf_{\theta>0}\Bigl\{e^{-\theta t}\cdot\operatorname{tr}\exp\Bigl(\sum_k\log\mathbb E\,e^{\theta X_k}\Bigr)\Bigr\}.P{λmax​(k∑​Xk​)≥t}≤θ>0inf​{e−θt⋅trexp(k∑​logEeθXk​)}.

It contains no constants and no assumption beyond independence: every later inequality of the paper specializes it.

Milestones

  1. Proposition 3.1 (Laplace transform method): P{λmax⁡(Y)≥t}≤inf⁡θ>0{e−θt Etr⁡eθY}\mathbb P\{\lambda_{\max}(Y)\ge t\}\le\inf_{\theta>0}\{e^{-\theta t}\,\mathbb E\operatorname{tr}e^{\theta Y}\}P{λmax​(Y)≥t}≤infθ>0​{e−θtEtreθY}.
  2. Theorem 3.2 (Lieb): for fixed self-adjoint HHH, A↦tr⁡exp⁡(H+log⁡A)A\mapsto\operatorname{tr}\exp(H+\log A)A↦trexp(H+logA) is concave on the positive-definite cone.
  3. Corollary 3.3: Etr⁡exp⁡(H+X)≤tr⁡exp⁡(H+log⁡E eX)\mathbb E\operatorname{tr}\exp(H+X)\le\operatorname{tr}\exp(H+\log\mathbb E\,e^{X})Etrexp(H+X)≤trexp(H+logEeX).
  4. Lemma 3.4 (subadditivity of matrix cgfs): Etr⁡exp⁡(∑kθXk)≤tr⁡exp⁡(∑klog⁡E eθXk)\mathbb E\operatorname{tr}\exp(\sum_k\theta X_k)\le\operatorname{tr}\exp(\sum_k\log\mathbb E\,e^{\theta X_k})Etrexp(∑k​θXk​)≤trexp(∑k​logEeθXk​) for θ∈R\theta\in\mathbb Rθ∈R.

Significance

The master bound reduces every tail estimate for λmax⁡\lambda_{\max}λmax​ of an independent sum to semidefinite bounds on the individual cumulant generating functions. The paper's matrix Gaussian and Rademacher series bound, matrix Chernoff inequality and matrix Bernstein inequality are each one such bound away from it, and the matrix Bernstein inequality in particular is a standard tool in randomized numerical linear algebra, matrix completion and covariance estimation. Missions II–IV of this series take the master bound as their first milestone.

All results here are proved in the literature. What remains is formalization: none of Lieb's concavity theorem, the matrix Laplace transform bound or the subadditivity of matrix cumulant generating functions is in Mathlib, and a machine-checked Lieb theorem would be reusable throughout quantum information theory (strong subadditivity of entropy, joint convexity of relative entropy).

Difficulty

The scalar argument factors Eexp⁡(∑kθXk)=∏kE eθXk\mathbb E\exp(\sum_k\theta X_k)=\prod_k\mathbb E\,e^{\theta X_k}Eexp(∑k​θXk​)=∏k​EeθXk​, which needs ea+b=eaebe^{a+b}=e^ae^bea+b=eaeb. For non-commuting matrices eA+B≠eAeBe^{A+B}\ne e^Ae^BeA+B=eAeB, so this step fails. The Golden–Thompson inequality tr⁡eA+H≤tr⁡(eAeH)\operatorname{tr}e^{A+H}\le\operatorname{tr}(e^Ae^H)treA+H≤tr(eAeH) handles two summands but its three-matrix analogue is false, so it does not iterate. Lieb's concavity theorem is the deep input; it does not follow from elementary properties of the exponential, which is neither operator monotone nor operator convex. On the formal side, the matrix functional calculus of Mathlib carries little of the trace-function theory the statements rely on.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ with [NeZero d] wherever λmax⁡\lambda_{\max}λmax​ appears; for d=0d=0d=0 the largest eigenvalue would be 000 and the bound would fail at t≤0t\le0t≤0. Exponential and logarithm are Mathlib's continuous functional calculus cfc. Random matrices are measurable maps for the Borel σ-algebra on the entries, independence is iIndepFun, and P is a probability measure. Expectation is entrywise.

The paper's standing assumption that expectations exist is made explicit and only where an expectation is taken: every entry of eθXke^{\theta X_k}eθXk​ is integrable for the θ\thetaθ in question. The infimum over θ>0\theta>0θ>0 is stated as the bound for every θ>0\theta>0θ>0 at which the moment generating functions exist; since an inequality p≤inf⁡θF(θ)p\le\inf_\theta F(\theta)p≤infθ​F(θ) is equivalent to p≤F(θ)p\le F(\theta)p≤F(θ) for every θ\thetaθ, and the paper treats a non-existent moment generating function as +∞+\infty+∞, this is exact. A real-valued infimum over θ\thetaθ, or dropping the integrability hypotheses, would make the statements trivially true through Lean's default values (inf⁡\infinf of an unbounded set and the integral of a non-integrable function are 000); the formalization rules both out.

Useful infrastructure beyond this mission: trace inequalities for cfc on Hermitian matrices, monotonicity of the trace exponential in the semidefinite order, and Lieb's concavity theorem itself. Contributions of any of these as standalone lemmas are welcome.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, arXiv:1004.4389v7 (2011); Found. Comput. Math. 12 (2012) 389–434. https://arxiv.org/abs/1004.4389, https://doi.org/10.1007/s10208-011-9099-z
  • R. Ahlswede and A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48(3) (2002) 569–579. https://arxiv.org/abs/quant-ph/0012127
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
  • H. Epstein, Remarks on two theorems of E. Lieb, Comm. Math. Phys. 31 (1973) 317–325. https://doi.org/10.1007/BF01646492
  • J. A. Tropp, From joint convexity of quantum relative entropy to a concavity theorem of Lieb, Proc. Amer. Math. Soc. 140 (2012) 1757–1760. https://arxiv.org/abs/1101.1070
6 thms2 active usersReviewed
Machine LearningProbabilityStatistics·Captain: mikedeng1

Nuclear-Norm Penalization and Optimal Rates for Noisy Low-Rank Matrix Completion 3: Uniform Matrix Completion with |Yᵢ| ≤ η — With Probability ≥ 1 − e^{−t} the Oracle Bound (3.5) Holds for All AResearch Paper

Motivation

Matrix completion asks to recover a large matrix from a small number of its entries. It is the abstraction behind collaborative filtering (recommender systems in which a users × items rating matrix is observed on a sparse set of pairs), sensor localization from partial distance information, and system identification. Without structure the problem is hopeless; the standard structural assumption is that the unknown matrix has low rank, and the standard convex surrogate for rank is the nuclear norm, the sum of singular values.

In the noiseless case, exact recovery by nuclear-norm minimization from about r(m1∨m2) polylogr(m_1\vee m_2)\,\mathrm{polylog}r(m1​∨m2​)polylog uniformly sampled entries was established by Candès and Recht (2009) and refined by Candès and Tao (2010) and Gross (2011). With noisy observations the relevant question is a rate: how fast does an estimator's error decrease with the number nnn of observed entries? Koltchinskii, Lounici and Tsybakov (arXiv:1011.6256, Ann. Statist. 2011) introduced a nuclear-norm penalized estimator that uses the known sampling distribution, showed that in matrix completion it is an explicit soft thresholding of the singular values of a rescaled data matrix, and proved for it sharp oracle inequalities (leading constant 1) whose rates are optimal up to logarithmic factors. This mission formalizes the version of that result for bounded responses: Theorem 4 of the paper, together with the probabilistic lemma and the matrix Bernstein inequality it rests on.

Setting

Fix positive integers n,m1,m2n, m_1, m_2n,m1​,m2​ and write Rm1×m2\mathbb R^{m_1\times m_2}Rm1​×m2​ for the real m1×m2m_1\times m_2m1​×m2​ matrices, with scalar product ⟨A,B⟩=tr⁡(A⊤B)\langle A,B\rangle=\operatorname{tr}(A^\top B)⟨A,B⟩=tr(A⊤B), Frobenius norm ∥A∥2\|A\|_2∥A∥2​, nuclear norm ∥A∥1\|A\|_1∥A∥1​ (sum of singular values) and operator norm ∥A∥∞\|A\|_\infty∥A∥∞​ (largest singular value). Set m=m1+m2m=m_1+m_2m=m1​+m2​ and write m1∧m2=min⁡(m1,m2)m_1\wedge m_2=\min(m_1,m_2)m1​∧m2​=min(m1​,m2​).

The matrix completion basis is

X={ej(m1)ek⊤(m2):1≤j≤m1, 1≤k≤m2},\mathcal X=\{e_j(m_1)e_k^\top(m_2):1\le j\le m_1,\ 1\le k\le m_2\},X={ej​(m1​)ek⊤​(m2​):1≤j≤m1​, 1≤k≤m2​},

where ek(m)e_k(m)ek​(m) are the canonical basis vectors of Rm\mathbb R^mRm. One observes nnn independent random pairs (Xi,Yi)(X_i,Y_i)(Xi​,Yi​), where XiX_iXi​ is uniformly distributed on X\mathcal XX and YiY_iYi​ is real, following the trace regression model

E(Yi∣Xi)=tr⁡(Xi⊤A0),\mathbb E(Y_i\mid X_i)=\operatorname{tr}(X_i^\top A_0),E(Yi​∣Xi​)=tr(Xi⊤​A0​),

for an unknown A0∈Rm1×m2A_0\in\mathbb R^{m_1\times m_2}A0​∈Rm1​×m2​. Thus YiY_iYi​ is a noisy reading of the entry of A0A_0A0​ selected by XiX_iXi​; this is matrix completion under uniform sampling at random (USR), entries possibly sampled more than once.

The estimator is, for a regularization parameter λ>0\lambda>0λ>0,

A^λ=argmin⁡A∈Rm1×m2(1m1m2∥A∥22−⟨2n∑i=1nYiXi,A⟩+λ∥A∥1).\hat A^\lambda=\operatorname*{argmin}_{A\in\mathbb R^{m_1\times m_2}}\Big(\frac1{m_1m_2}\|A\|_2^2-\Big\langle\frac2n\sum_{i=1}^nY_iX_i,A\Big\rangle+\lambda\|A\|_1\Big).A^λ=A∈Rm1​×m2​argmin​(m1​m2​1​∥A∥22​−⟨n2​i=1∑n​Yi​Xi​,A⟩+λ∥A∥1​).

The stochastic error is the random matrix

M=1n∑i=1n(YiXi−E(YiXi)).\mathbf M=\frac1n\sum_{i=1}^n\big(Y_iX_i-\mathbb E(Y_iX_i)\big).M=n1​i=1∑n​(Yi​Xi​−E(Yi​Xi​)).

Formalization targets

Goal: Theorem 4

Assume max⁡i∣Yi∣≤η\max_i|Y_i|\le\etamaxi​∣Yi​∣≤η almost surely. For t>0t>0t>0 and

λ≥4ηmax⁡{t+log⁡m(m1∧m2)n, 2(t+log⁡m)n},\lambda\ge4\eta\max\Big\{\sqrt{\frac{t+\log m}{(m_1\wedge m_2)n}},\ \frac{2(t+\log m)}{n}\Big\},λ≥4ηmax{(m1​∧m2​)nt+logm​​, n2(t+logm)​},

with probability at least 1−e−t1-e^{-t}1−e−t, simultaneously for all A∈Rm1×m2A\in\mathbb R^{m_1\times m_2}A∈Rm1​×m2​,

∥A^λ−A0∥22≤∥A−A0∥22+m1m2min⁡{2λ∥A∥1, (1+22)2m1m2λ2rank⁡(A)}.\|\hat A^\lambda-A_0\|_2^2\le\|A-A_0\|_2^2+m_1m_2\min\Big\{2\lambda\|A\|_1,\ \Big(\frac{1+\sqrt2}2\Big)^2m_1m_2\lambda^2\operatorname{rank}(A)\Big\}.∥A^λ−A0​∥22​≤∥A−A0​∥22​+m1​m2​min{2λ∥A∥1​, (21+2​​)2m1​m2​λ2rank(A)}.

Milestones

  1. (1.4): ∥A∥L2(Π)2=1n∑iE⟨A,Xi⟩2=(m1m2)−1∥A∥22\|A\|_{L_2(\Pi)}^2=\frac1n\sum_i\mathbb E\langle A,X_i\rangle^2=(m_1m_2)^{-1}\|A\|_2^2∥A∥L2​(Π)2​=n1​∑i​E⟨A,Xi​⟩2=(m1​m2​)−1∥A∥22​ for the uniform design.
  2. Theorem 1 for USR matrix completion: at every sample point where λ≥2∥M∥∞\lambda\ge2\|\mathbf M\|_\inftyλ≥2∥M∥∞​, the inequality above holds for all AAA (a deterministic statement).
  3. Proposition 1 (matrix Bernstein): for independent centred m1×m2m_1\times m_2m1​×m2​ random matrices ZiZ_iZi​ with ∥Zi∥≤U\|Z_i\|\le U∥Zi​∥≤U a.s., with probability at least 1−e−t1-e^{-t}1−e−t,
∥Z1+⋯+Znn∥≤2max⁡{σZt+log⁡mn, Ut+log⁡mn}.\Big\|\frac{Z_1+\dots+Z_n}n\Big\|\le2\max\Big\{\sigma_Z\sqrt{\frac{t+\log m}n},\ U\frac{t+\log m}n\Big\}.​nZ1​+⋯+Zn​​​≤2max{σZ​nt+logm​​, Unt+logm​}.
  1. (6.2): for XXX uniform on X\mathcal XX, ∥X∥=1\|X\|=1∥X∥=1, ∥EX∥=(m1m2)−1/2\|\mathbb EX\|=(m_1m_2)^{-1/2}∥EX∥=(m1​m2​)−1/2, σX2=1/(m1∧m2)\sigma_X^2=1/(m_1\wedge m_2)σX2​=1/(m1​∧m2​).
  2. Lemma 1: with probability at least 1−e−t1-e^{-t}1−e−t, ∥M∥≤2ηmax⁡{(t+log⁡m)/((m1∧m2)n), 2(t+log⁡m)/n}\|\mathbf M\|\le2\eta\max\{\sqrt{(t+\log m)/((m_1\wedge m_2)n)},\ 2(t+\log m)/n\}∥M∥≤2ηmax{(t+logm)/((m1​∧m2​)n)​, 2(t+logm)/n}.

Significance

Theorem 4 is a non-asymptotic, sharp oracle inequality: the leading constant in front of ∥A−A0∥22\|A-A_0\|_2^2∥A−A0​∥22​ is 1, so the bound applies to misspecified targets (A0A_0A0​ not low rank) without loss. Taking A=A0A=A_0A=A0​ and ttt of order log⁡m\log mlogm gives a normalized Frobenius error of order η2(m1∨m2)rank⁡(A0)log⁡(m)/n\eta^2(m_1\vee m_2)\operatorname{rank}(A_0)\log(m)/nη2(m1​∨m2​)rank(A0​)log(m)/n, which the paper's minimax lower bounds (§4) show to be optimal up to the logarithm. Because no model is needed for Lemma 1, the same probability bound also drives the paper's statistical-learning reformulation (Theorem 9).

The theorems here are proved in the paper. What is open is their formalization: no matrix Bernstein inequality, and no oracle inequality for nuclear-norm penalized estimators, has a machine-checked proof on this platform. Proposition 1 in particular is a reusable concentration tool well beyond this paper (covariance estimation, random graphs, sketching).

Difficulty

The deterministic part (milestone 2) needs the subdifferential of the nuclear norm, which is not in Mathlib. The probabilistic part is where the obvious argument fails. Bounding ∥M∥∞\|\mathbf M\|_\infty∥M∥∞​ entrywise and summing, or bounding it by the Frobenius norm, loses a factor polynomial in the dimension; a union bound over a net of the unit sphere loses the factor m1∧m2m_1\wedge m_2m1​∧m2​ that makes the rate optimal. The correct rate requires a noncommutative Bernstein inequality, controlling the operator norm of a sum of independent random matrices through the matrix variance σZ2\sigma_Z^2σZ2​ at the price of only a log⁡(m1+m2)\log(m_1+m_2)log(m1​+m2​) factor. The matrix-analytic machinery such inequalities depend on (trace inequalities for matrix exponentials, the passage from rectangular to symmetric matrices) is not currently available in Mathlib.

Formalization scope

All objects are local to the namespace KLTNuclear.Completion, built on the published MatrixCompletion definitions (RealMatrix, nuclearNorm, spectralNorm, frobeniusNormSq, matrixInner, coordinateMatrix). Conventions:

  • The probability space carries IsProbabilityMeasure; n,m1,m2≥1n,m_1,m_2\ge1n,m1​,m2​≥1 are hypotheses. log⁡\loglog is the natural logarithm; m=m1+m2≥2m=m_1+m_2\ge2m=m1​+m2​≥2.
  • The design is encoded by uniform random indices Ii∈[m1]×[m2]I_i\in[m_1]\times[m_2]Ii​∈[m1​]×[m2​] with Xi=ejieki⊤X_i=e_{j_i}e_{k_i}^\topXi​=eji​​eki​⊤​. Mathlib has no σ\sigmaσ-algebra on Matrix, so measurability, independence and conditioning on a random matrix use its entry array with the product σ\sigmaσ-algebra; expectations of matrices are entrywise.
  • The model (1.1) is a conditional expectation given σ(Xi)\sigma(X_i)σ(Xi​). Independence of the pairs (Xi,Yi)(X_i,Y_i)(Xi​,Yi​) is the paper's standing assumption (p. 1) and is assumed in Lemma 1 and Theorem 4, whose proof applies Proposition 1 to Zi=YiXi−E(YiXi)Z_i=Y_iX_i-\mathbb E(Y_iX_i)Zi​=Yi​Xi​−E(Yi​Xi​); the YiY_iYi​ are not assumed identically distributed. λ>0\lambda>0λ>0 is the standing assumption of (1.6). Integrable responses are assumed in milestone 2, bounded measurable responses in Lemma 1 and Theorem 4.
  • A^λ\hat A^\lambdaA^λ is any minimizer of (3.1) at each sample point (it exists and is unique, but neither fact is assumed); the soft-thresholding formula (3.2) is not used as a definition.
  • "With probability at least 1−e−t1-e^{-t}1−e−t" is encoded as an upper bound e−te^{-t}e−t on the outer measure of the failure set; in Theorem 4 the failure set is {ω:∃A, (3.5) fails}\{\omega:\exists A,\ \text{(3.5) fails}\}{ω:∃A, (3.5) fails}, so the bound is uniform in AAA. A formalization that fixes AAA before the probability is weaker and is not the target.
  • No printed slip affects these statements; Corollary 2(ii) of the paper, whose λ\lambdaλ falls below (3.6), is deliberately not included.

The source is the arXiv preprint arXiv:1011.6256v4. Welcome contributions: a general matrix Bernstein inequality (Hermitian and rectangular forms), the nuclear-norm subdifferential, and proofs of the deterministic milestone.

Selected references

  • V. Koltchinskii, K. Lounici, A. B. Tsybakov, Nuclear-norm penalization and optimal rates for noisy low-rank matrix completion, Ann. Statist. 39(5), 2011; preprint arXiv:1011.6256v4. https://arxiv.org/abs/1011.6256
  • J. A. Tropp, User-friendly tail bounds for sums of random matrices, Found. Comput. Math. 12, 2012. https://doi.org/10.1007/s10208-011-9099-z
  • E. J. Candès, B. Recht, Exact matrix completion via convex optimization, Found. Comput. Math. 9, 2009. https://doi.org/10.1007/s10208-009-9045-5
  • E. J. Candès, T. Tao, The power of convex relaxation: near-optimal matrix completion, IEEE Trans. Inform. Theory 56, 2010. https://doi.org/10.1109/TIT.2010.2044061
  • D. Gross, Recovering low-rank matrices from few coefficients in any basis, IEEE Trans. Inform. Theory 57, 2011. https://doi.org/10.1109/TIT.2011.2104999
12 thms2 active usersReviewed
ProbabilityStatistics·Captain: mikedeng1

Phase Transition of the Largest Eigenvalue for Nonnull Complex Sample Covariance Matrices 3: With N = k Variables Fixed and Equal Population Eigenvalues, √M(λ₁ − ℓ₁)/ℓ₁ Converges to G_kResearch Paper

Motivation

Principal component analysis estimates the eigenvalues of a population covariance matrix Σ\SigmaΣ by those of the sample covariance matrix SSS. Before random matrix theory turned to the regime where the dimension grows with the sample size, the classical question was the opposite one: the number of variables NNN is fixed and the number of samples MMM tends to infinity. In that regime S→ΣS\to\SigmaS→Σ almost surely, and the next question is the size and shape of the fluctuations of the sample eigenvalues. When Σ\SigmaΣ has a repeated eigenvalue, the sample eigenvalues near it do not fluctuate independently: they repel each other, and their joint limit law is that of the eigenvalues of a random Hermitian (or symmetric) matrix. Anderson (1963) derived these limits for real Gaussian samples.

Baik, Ben Arous and Péché (2005) study complex Gaussian samples whose covariance matrix is the identity apart from finitely many "spiked" eigenvalues, and find a phase transition for the largest sample eigenvalue λ1\lambda_1λ1​ as M,N→∞M,N\to\inftyM,N→∞ together. Their Proposition 1.1 is the fixed-dimension counterpart: with N=kN=kN=k fixed and all population eigenvalues equal, λ1\lambda_1λ1​ fluctuates on the scale M−1/2M^{-1/2}M−1/2 with the law of the largest eigenvalue of a k×kk\times kk×k Gaussian unitary ensemble (GUE). The paper places it beside its Theorem 1.1(b), where a kkk-fold spike above the critical value 1+γ−11+\gamma^{-1}1+γ−1 gives the same GUE limit when N→∞N\to\inftyN→∞. This mission formalizes Proposition 1.1.

Setting

Fix k≥1k\ge1k≥1 and ℓ1>0\ell_1>0ℓ1​>0. A standard complex Gaussian is g=a+ibg=a+ibg=a+ib with a,ba,ba,b independent centred real Gaussians of variance 1/21/21/2, so E∣g∣2=1\mathbb E|g|^2=1E∣g∣2=1. For each MMM, let G=(Gmj)G=(G_{mj})G=(Gmj​), 1≤m≤M1\le m\le M1≤m≤M, 1≤j≤k1\le j\le k1≤j≤k, have independent standard complex Gaussian entries (sampleLaw M k), and let the samples be y⃗m=ℓ1 (Gm1,…,Gmk)T\vec y_m=\sqrt{\ell_1}\,(G_{m1},\dots,G_{mk})^{\mathsf T}y​m​=ℓ1​​(Gm1​,…,Gmk​)T: mean zero, covariance Σ=ℓ1Ik\Sigma=\ell_1 I_kΣ=ℓ1​Ik​. The sample covariance matrix is

S=1M∑m=1My⃗m y⃗m ∗,S=\frac1M\sum_{m=1}^M\vec y_m\,\vec y_m^{\,*},S=M1​m=1∑M​y​m​y​m∗​,

a k×kk\times kk×k Hermitian matrix (sampleCov), and λ1\lambda_1λ1​ is its largest eigenvalue (largestEig). The general model sampleVec U ℓ G m =Udiag⁡(ℓ) g⃗m=U\operatorname{diag}(\sqrt{\ell})\,\vec g_m=Udiag(ℓ​)g​m​ is specialized to U=IU=IU=I and ℓj=ℓ1\ell_j=\ell_1ℓj​=ℓ1​, because a Hermitian matrix with all eigenvalues equal to ℓ1\ell_1ℓ1​ is ℓ1Ik\ell_1 I_kℓ1​Ik​.

Write V(ξ)2=∏1≤i<j≤k∣ξi−ξj∣2V(\xi)^2=\prod_{1\le i<j\le k}|\xi_i-\xi_j|^2V(ξ)2=∏1≤i<j≤k​∣ξi​−ξj​∣2 (vandSq). The finite-GUE distribution (Definition 1.2) is

Gk(x)=1Zk∫(−∞,x]kV(ξ)2∏i=1ke−ξi2/2 dξ,Zk=∫RkV(ξ)2∏i=1ke−ξi2/2 dξ,G_k(x)=\frac1{Z_k}\int_{(-\infty,x]^k}V(\xi)^2\prod_{i=1}^ke^{-\xi_i^2/2}\,d\xi,\qquad Z_k=\int_{\mathbb R^k}V(\xi)^2\prod_{i=1}^ke^{-\xi_i^2/2}\,d\xi,Gk​(x)=Zk​1​∫(−∞,x]k​V(ξ)2i=1∏k​e−ξi2​/2dξ,Zk​=∫Rk​V(ξ)2i=1∏k​e−ξi2​/2dξ,

the distribution function of the largest eigenvalue of a k×kk\times kk×k GUE matrix. In Lean these are G k x and Z k.

Formalization targets

Goal: Proposition 1.1

For every real xxx and every ε>0\varepsilon>0ε>0,

lim⁡M→∞P((λ1−ℓ1)1ℓ1M≤x)=Gk(x),lim⁡M→∞P(∣λ1−ℓ1∣>ε)=0.\lim_{M\to\infty}\mathbb P\Big((\lambda_1-\ell_1)\frac1{\ell_1}\sqrt M\le x\Big)=G_k(x),\qquad \lim_{M\to\infty}\mathbb P\big(|\lambda_1-\ell_1|>\varepsilon\big)=0 .M→∞lim​P((λ1​−ℓ1​)ℓ1​1​M​≤x)=Gk​(x),M→∞lim​P(∣λ1​−ℓ1​∣>ε)=0.

The second statement is λ1→ℓ1\lambda_1\to\ell_1λ1​→ℓ1​ in probability.

Milestones

With π1=ℓ1−1\pi_1=\ell_1^{-1}π1​=ℓ1−1​, M≥kM\ge kM≥k, and C=∫(0,∞)kV(y)2∏je−Mπ1yjyjM−k dyC=\int_{(0,\infty)^k}V(y)^2\prod_je^{-M\pi_1y_j}y_j^{M-k}\,dyC=∫(0,∞)k​V(y)2∏j​e−Mπ1​yj​yjM−k​dy:

  1. (302) P(λ1≤t)=1C∫(0,t]kV(y)2∏je−Mπ1yjyjM−k dy\mathbb P(\lambda_1\le t)=\frac1C\int_{(0,t]^k}V(y)^2\prod_je^{-M\pi_1y_j}y_j^{M-k}\,dyP(λ1​≤t)=C1​∫(0,t]k​V(y)2∏j​e−Mπ1​yj​yjM−k​dy;
  2. (303) C=∏j=0k−1(1+j)!(M−k+j)! / (Mπ1)MkC=\prod_{j=0}^{k-1}(1+j)!(M-k+j)!\,/\,(M\pi_1)^{Mk}C=∏j=0k−1​(1+j)!(M−k+j)!/(Mπ1​)Mk;
  3. (27) Zk=(2π)k/2∏j=1kj!Z_k=(2\pi)^{k/2}\prod_{j=1}^kj!Zk​=(2π)k/2∏j=1k​j!;
  4. (304) the rescaled form of (302) after yj=π1−1(1+ξj/M)y_j=\pi_1^{-1}(1+\xi_j/\sqrt M)yj​=π1−1​(1+ξj​/M​);
  5. π1kMMk2/2ekMC→(2π)k/2∏j=0k−1(1+j)!\pi_1^{kM}M^{k^2/2}e^{kM}C\to(2\pi)^{k/2}\prod_{j=0}^{k-1}(1+j)!π1kM​Mk2/2ekMC→(2π)k/2∏j=0k−1​(1+j)! as M→∞M\to\inftyM→∞;
  6. (29) G1G_1G1​ is the standard normal distribution function.

Significance

The proposition identifies the fixed-dimension limit of the top sample eigenvalue under a degenerate population spectrum: the kkk sample eigenvalues near ℓ1\ell_1ℓ1​, rescaled by M/ℓ1\sqrt M/\ell_1M​/ℓ1​, behave like a k×kk\times kk×k GUE spectrum, and λ1\lambda_1λ1​ like its maximum. For k=1k=1k=1 it reduces to the central limit theorem for the sample variance of one complex Gaussian variable, with limit Φ\PhiΦ by (29). For general kkk it shows that the GUE limit of the supercritical regime in Theorem 1.1(b) is already present when the dimension does not grow.

The result is proved in the paper (§5, p. 1691) by an exact computation. No machine-checked proof of it, of the complex Wishart eigenvalue density, or of the Gaussian and Laguerre cases of Selberg's integral is known to exist in Mathlib or on the platform. The formalization requires the joint eigenvalue density of a complex Wishart matrix (a Weyl-type integration formula over the unitary group), two Selberg-type integral evaluations, a Stirling asymptotic for products of factorials, and a dominated-convergence argument on Rk\mathbb R^kRk. The first three are reusable well beyond this mission.

Difficulty

The limit itself follows from (304) and the constant asymptotics. The hard part is (302): passing from the law of the matrix SSS to the joint law of its eigenvalues. This requires the change of variables S=Wdiag⁡(λ)W∗S=W\operatorname{diag}(\lambda)W^*S=Wdiag(λ)W∗ with WWW unitary, the Jacobian V(λ)2V(\lambda)^2V(λ)2, and the integration over the unitary group. A direct central limit argument for the entries of SSS gives the Gaussian limit of M(S−ℓ1I)/ℓ1\sqrt M(S-\ell_1I)/\ell_1M​(S−ℓ1​I)/ℓ1​ as a GUE matrix. To get from there to λ1\lambda_1λ1​ one needs the continuity of the largest eigenvalue in the matrix entries and a matching normalisation, so it is a different route from the paper's. Either route requires spectral facts about Hermitian matrices that Mathlib does not yet package. The Selberg evaluations (27) and (303) are classical but have no short proof: the standard arguments use orthogonal polynomials or an induction with a Dixon–Anderson type integral.

Formalization scope

  • The sample model is shared by every mission of this series:
    • the samples are mean-zero and uncentred, with E∣g∣2=1\mathbb E|g|^2=1E∣g∣2=1 per complex coordinate, and SSS carries the factor 1/M1/M1/M, as in the paper's formula (59). The density (1) "with the complex inner product", S=1NXX∗S=\frac1NXX^*S=N1​XX∗ on p. 1645 and the centring by the sample mean on p. 1643 are printed slips that contradict (59);
    • λ1\lambda_1λ1​ is the supremum of Mathlib's eigenvalues of the Hermitian matrix SSS. The events {λ1≤t}\{\lambda_1\le t\}{λ1​≤t} are closed, hence measurable, sets of samples.
  • The probabilities are (sampleLaw M k).real of explicit sets.
  • (50) is printed without "≤\le≤"; the event (λ1−ℓ1)ℓ1−1M≤x(\lambda_1-\ell_1)\ell_1^{-1}\sqrt M\le x(λ1​−ℓ1​)ℓ1−1​M​≤x is stated.
  • (29) is printed with "erf(x)"; the standard normal distribution function is stated.
  • ZkZ_kZk​ and CCC are defined as integrals, never as their closed forms. Otherwise (27) and (303) would hold by definition.
  • The goal mentions only the sample model, λ1\lambda_1λ1​ and GkG_kGk​, not CCC, the Laguerre weight or the substitution. This rules out the trivializing formalizations: the covariance is the page's ℓ1Ik\ell_1I_kℓ1​Ik​, not a further special case, and nothing in the statement is vacuous for k≥1k\ge1k≥1, ℓ1>0\ell_1>0ℓ1​>0.
  • The milestones (302)–(304) assume k≤Mk\le Mk≤M, which the page uses implicitly through the exponent M−kM-kM−k. (304) assumes x≥−Mx\ge-\sqrt Mx≥−M​, the range of its integration limits.

Contributions are welcome on each milestone. Particularly reusable are the complex Wishart eigenvalue density, the Gaussian and Laguerre Selberg integrals, and the measurability and continuity of eigenvalues of Hermitian matrix families.

Selected references

  • J. Baik, G. Ben Arous, S. Péché, Phase transition of the largest eigenvalue for nonnull complex sample covariance matrices, Ann. Probab. 33(5) (2005), 1643–1697. https://doi.org/10.1214/009117905000000233
  • T. W. Anderson, Asymptotic theory for principal component analysis, Ann. Math. Statist. 34 (1963), 122–148. https://doi.org/10.1214/aoms/1177704248
  • A. T. James, Distributions of matrix variates and latent roots derived from normal samples, Ann. Math. Statist. 35 (1964), 475–501. https://doi.org/10.1214/aoms/1177703550
  • I. M. Johnstone, On the distribution of the largest eigenvalue in principal components analysis, Ann. Statist. 29 (2001), 295–327. https://doi.org/10.1214/aos/1009210544
  • P. J. Forrester, S. O. Warnaar, The importance of the Selberg integral, Bull. Amer. Math. Soc. 45 (2008), 489–534. https://doi.org/10.1090/S0273-0979-08-01221-4
11 thms2 active usersReviewed
Convex OptimizationStatistics·Captain: mikedeng1

Robust Principal Component Analysis?: Principal Component Pursuit with λ = 1/√n Exactly Recovers an Incoherent Low-Rank Matrix from a Constant Fraction of Randomly Located Gross ErrorsResearch Paper

Motivation

Principal component analysis finds the best low-rank approximation of a data matrix, and it is used everywhere data come as a table: images, video, genomics, web and survey data. Its weakness is well known: a single grossly corrupted entry can move the classical principal components arbitrarily far. In many applications the corruptions are not small noise but gross errors at a fraction of the entries: occlusions and specularities in face images, moving foreground objects in surveillance video, corrupted or adversarial records. Robust variants of PCA built on robust statistics or on alternating heuristics came without guarantees of exact recovery.

Candès, Li, Ma and Wright (J. ACM 58(3), 2011) showed that a single convex program recovers both the low-rank part and the corruptions exactly, under a randomness assumption on the corruption pattern only, with a weight that needs no tuning.

Timeline.

  • 2009: Candès and Recht prove exact matrix completion by nuclear-norm minimization under incoherence (FoCM 2009). Their concentration results reappear here as Theorem 2.6 and Lemma 3.2.
  • 2009: Chandrasekaran, Sanghavi, Parrilo and Willsky give deterministic conditions for the same convex decomposition (SIAM J. Optim. 2011, arXiv:0906.2220). As compared on p. 7 of the present paper, these conditions allow only a vanishing fraction O((nr)−1/2)O((nr)^{-1/2})O((nr)−1/2) of corrupted entries, and they leave the weight λ\lambdaλ to be searched for.
  • 2009: Gross introduces the golfing scheme for constructing dual certificates (IEEE Trans. Inf. Theory 2011, arXiv:0910.1879). This paper adapts it.
  • 2009–2011: the present paper (preprint of 17 December 2009) proves Theorem 1.1: a constant fraction of corrupted entries and rank up to n/(log⁡n)2n/(\log n)^2n/(logn)2.

Setting

Let L0∈Rn×nL_0\in\mathbb R^{n\times n}L0​∈Rn×n have rank rrr and compact singular value decomposition L0=∑k=1rσkukvk∗L_0=\sum_{k=1}^r\sigma_k u_kv_k^*L0​=∑k=1r​σk​uk​vk∗​ with σk>0\sigma_k>0σk​>0, where U=[u1,…,ur]U=[u_1,\dots,u_r]U=[u1​,…,ur​] and V=[v1,…,vr]V=[v_1,\dots,v_r]V=[v1​,…,vr​] have orthonormal columns. The nuclear norm ∥M∥∗\|M\|_*∥M∥∗​ is the sum of the singular values of MMM, and ∥M∥1=∑ij∣Mij∣\|M\|_1=\sum_{ij}|M_{ij}|∥M∥1​=∑ij​∣Mij​∣ is the entrywise ℓ1\ell_1ℓ1​ norm. Given M=L0+S0M=L_0+S_0M=L0​+S0​, Principal Component Pursuit (PCP) solves

minimize  ∥L∥∗+λ∥S∥1subject toL+S=M.(1.1)\text{minimize }\ \|L\|_*+\lambda\|S\|_1\qquad\text{subject to}\qquad L+S=M. \tag{1.1}minimize  ∥L∥∗​+λ∥S∥1​subject toL+S=M.(1.1)

PCP is exact when (L0,S0)(L_0,S_0)(L0​,S0​) is its unique solution.

L0L_0L0​ satisfies the incoherence condition with parameter μ\muμ when

max⁡i∥U∗ei∥2≤μrn,max⁡i∥V∗ei∥2≤μrn,∥UV∗∥∞≤μrn2,(1.2–1.3)\max_i\|U^*e_i\|^2\le\frac{\mu r}{n},\qquad\max_i\|V^*e_i\|^2\le\frac{\mu r}{n},\qquad\|UV^*\|_\infty\le\sqrt{\frac{\mu r}{n^2}},\tag{1.2–1.3}imax​∥U∗ei​∥2≤nμr​,imax​∥V∗ei​∥2≤nμr​,∥UV∗∥∞​≤n2μr​​,(1.2–1.3)

where ∥X∥∞=max⁡ij∣Xij∣\|X\|_\infty=\max_{ij}|X_{ij}|∥X∥∞​=maxij​∣Xij​∣. This excludes low-rank matrices that are themselves sparse, which no method could tell apart from corruptions.

The sparse component is S0=PΩSS_0=\mathcal P_\Omega SS0​=PΩ​S, where SSS is an arbitrary fixed matrix and PΩ\mathcal P_\OmegaPΩ​ keeps the entries in a random support Ω\OmegaΩ and zeros the others. In Theorem 1.1, Ω\OmegaΩ is uniform among all subsets of [n]×[n][n]\times[n][n]×[n] of cardinality mmm. In the Bernoulli model Ω∼Ber(ρ)\Omega\sim\mathrm{Ber}(\rho)Ω∼Ber(ρ) each entry belongs to Ω\OmegaΩ independently with probability ρ\rhoρ. Nothing is assumed about the magnitudes or signs of SSS.

The proof works with the tangent space T={UX∗+YV∗}T=\{UX^*+YV^*\}T={UX∗+YV∗} of the rank-rrr matrices at L0L_0L0​, its orthogonal projections PT\mathcal P_TPT​ and PT⊥\mathcal P_{T^\perp}PT⊥​, and the operator norm ∥⋅∥\|\cdot\|∥⋅∥ (largest singular value).

Formalization targets

Goal: Theorem 1.1, square case

There are positive numerical constants c,ρr,ρsc,\rho_r,\rho_sc,ρr​,ρs​ such that, whenever L0L_0L0​ obeys (1.2)–(1.3) and

rank⁡(L0)≤ρr n μ−1(log⁡n)−2andm≤ρs n2,(1.4)\operatorname{rank}(L_0)\le\rho_r\,n\,\mu^{-1}(\log n)^{-2}\qquad\text{and}\qquad m\le\rho_s\,n^2,\tag{1.4}rank(L0​)≤ρr​nμ−1(logn)−2andm≤ρs​n2,(1.4)

PCP with λ=1/n\lambda=1/\sqrt nλ=1/n​ is exact with probability at least 1−c n−101-c\,n^{-10}1−cn−10 over the support of S0S_0S0​.

The constants are not specified, so the goal survives any improvement of them.

Milestones

They are listed in the order the proof uses them:

  • the coordinate bound (2.2);
  • the elimination theorem (Theorem 2.2): exactness passes to trimmed sparse components;
  • the transfer from the Bernoulli model to the uniform model (§7.1);
  • derandomization (Theorem 2.3): random signs suffice;
  • the dual certificate conditions (Lemma 2.4, Lemma 2.5, (2.4));
  • the concentration results (Theorem 2.6, Corollary 2.7, Lemmas 3.1 and 3.2);
  • the two halves of the certificate: the golfing certificate WLW^LWL (Lemma 2.8) and the least-squares certificate WSW^SWS (Lemma 2.9).

Significance

The result. Theorem 1.1 is the founding guarantee of robust PCA by convex optimization. It allows a constant fraction of arbitrarily large corruptions and a rank as large as n/(log⁡n)2n/(\log n)^2n/(logn)2, with a universal weight λ=1/n\lambda=1/\sqrt nλ=1/n​. It supports applications such as background modeling in video and the removal of shadows and specularities from face images, and it is the template for later work on noisy and partially observed variants, e.g. stable PCP (Zhou et al., ISIT 2010, arXiv:1001.2363).

Formalizing it. The theorem is proved on paper; no machine-checked proof of it is known. A formal proof would check a chain that combines convex duality for the nuclear and ℓ1\ell_1ℓ1​ norms, operator concentration for random sampling, and a probabilistic coupling. The reusable parts are general: the elimination and derandomization arguments, the certificate lemmas, the golfing scheme and the Bernoulli-to-uniform transfer. They also serve matrix completion and other sparse-plus-low-rank problems. The matrix-completion definitions this mission builds on are already published on the platform.

Difficulty

The obvious plan is to write down the subgradient optimality conditions of (1.1) and exhibit a dual certificate. The difficulty is the exact certificate (2.3). It requires PΩ(UV∗+W)=λsgn⁡(S0)\mathcal P_\Omega(UV^*+W)=\lambda\operatorname{sgn}(S_0)PΩ​(UV∗+W)=λsgn(S0​) exactly, and at the same time ∥W∥<1\|W\|<1∥W∥<1 and ∥PΩ⊥(UV∗+W)∥∞<λ\|\mathcal P_{\Omega^\perp}(UV^*+W)\|_\infty<\lambda∥PΩ⊥​(UV∗+W)∥∞​<λ, with Ω\OmegaΩ a constant fraction of all entries. The natural least-squares candidate cannot be controlled in the sup norm on Ω⊥\Omega^\perpΩ⊥ by moment methods at this sparsity level.

A second difficulty is probabilistic. The theorem allows fixed, adversarial signs. The concentration tools need independence, which fixed signs do not give.

Finally, every step must hold uniformly with failure probability O(n−10)O(n^{-10})O(n−10) and with constants independent of nnn, L0L_0L0​ and SSS.

Formalization scope

All statements are for square real matrices RealMatrix n n. The rectangular sentences of the paper are not stated. The mission reuses the published matrix-completion definitions for the following objects:

  • the nuclear norm (sum of Mathlib singular values);
  • the operator norm;
  • the Frobenius norm and inner product;
  • ∥⋅∥∞\|\cdot\|_\infty∥⋅∥∞​ and PΩ\mathcal P_\OmegaPΩ​;
  • SVD data SVD L0 r, with UV∗UV^*UV∗ = signMatrix;
  • PT\mathcal P_TPT​ and PT⊥\mathcal P_{T^\perp}PT⊥​;
  • the Bernoulli and uniform laws on supports.

The following conventions are fixed:

  • Rank. The rank is carried by SVD data SVD L0 r with positive singular values, so r=rank⁡L0r=\operatorname{rank}L_0r=rankL0​. Every statement holds for every such decomposition.
  • Exactness. "Exact" means unique optimality: every other feasible pair has a strictly larger objective.
  • Probabilities. Probabilities are finite sums of product weights. Operator norms of operators on matrices are taken with respect to the Frobenius norm.
  • Rank condition. It is written multiplied out, rμ(log⁡n)2≤ρrnr\mu(\log n)^2\le\rho_rnrμ(logn)2≤ρr​n, with the natural logarithm.
  • Constants. "With high probability" means probability at least 1−c n−101-c\,n^{-10}1−cn−10, with ccc a numerical constant. Every numerical constant is quantified before nnn, the matrices and the parameters.
  • Least-squares certificate. WSW^SWS is defined by the Neumann series (2.7), which the paper gives as an equivalent definition of (2.6), and it is used only on the event ∥PΩPT∥<1/2\|\mathcal P_\Omega\mathcal P_T\|<1/2∥PΩ​PT​∥<1/2.
  • Golfing. The golfing sets are indexed from 000.
  • Citations. Theorem numbers and pages are those of the preprint dated 17 December 2009, which is the cited source of the J. ACM article.

Trivializing formalizations are excluded. A constant ccc chosen after nnn would make the goal vacuous, so all constants come first. A non-strict "optimal" would make exactness much weaker, so exactness is strict. The values of S0S_0S0​ are fixed before the support is drawn.

Contributions of any kind are welcome. Proofs of the deterministic milestones (Theorem 2.2, Lemmas 2.4 and 2.5, (2.4), (2.2)) are self-contained convex analysis and linear algebra. The concentration milestones need matrix Bernstein-type inequalities and operator concentration, which are reusable well beyond this mission.

Selected references

  • E. J. Candès, X. Li, Y. Ma, J. Wright, Robust principal component analysis?, Journal of the ACM 58(3), Article 11, 2011. https://doi.org/10.1145/1970392.1970395
  • E. J. Candès, B. Recht, Exact matrix completion via convex optimization, Foundations of Computational Mathematics 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 Transactions on Information Theory 57(3), 1548–1566, 2011. https://arxiv.org/abs/0910.1879
  • V. Chandrasekaran, S. Sanghavi, P. A. Parrilo, A. S. Willsky, Rank-sparsity incoherence for matrix decomposition, SIAM Journal on Optimization 21(2), 572–596, 2011. https://arxiv.org/abs/0906.2220
  • Z. Zhou, X. Li, J. Wright, E. J. Candès, Y. Ma, Stable principal component pursuit, ISIT 2010. https://arxiv.org/abs/1001.2363
20 thms2 active usersReviewed
Dynamical SystemsOperations ResearchProbability·Captain: mikedeng1

Subadditive Ergodic Theory 5: For a Stationary Sequence in a Banach Algebra with E(log‖Y₁‖)⁺ < ∞, n⁻¹ log‖Y₁⋯Y_n‖ Converges in [−∞, ∞)Research Paper

Motivation

Products of random linear operators appear wherever a system evolves by repeated application of randomly chosen linear maps: linear recursions with random coefficients, products of random matrices in statistical physics, the growth of random dynamical systems, and population models in random environments. The basic question is the exponential growth rate of the product Y1Y2⋯YnY_1Y_2\cdots Y_nY1​Y2​⋯Yn​. For square matrices, Furstenberg and Kesten (Ann. Math. Statist. 31, 1960) proved that n−1log⁡∥Y1⋯Yn∥n^{-1}\log\|Y_1\cdots Y_n\|n−1log∥Y1​⋯Yn​∥ converges for stationary sequences with a logarithmic moment condition.

Kingman (Subadditive ergodic theory, Ann. Probab. 1(6):883–899, 1973) showed that this limit theorem is an instance of the subadditive ergodic theorem, and that the instance needs nothing of matrices beyond the norm inequality ∥AB∥≤∥A∥ ∥B∥\|AB\|\le\|A\|\,\|B\|∥AB∥≤∥A∥∥B∥. His Theorem 6 therefore holds in an arbitrary real or complex Banach algebra, including infinite-dimensional ones such as infinite matrices with finite ℓ1\ell_1ℓ1​ norm. It is the source of what later became known as the top Lyapunov exponent of a stationary random operator product.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space. A two-parameter family is a collection x=(xst)x=(x_{st})x=(xst​) of random variables indexed by nonnegative integers s<ts<ts<t. Kingman's conditions (§1.1–1.2) are:

  • S₁: xsu≤xst+xtux_{su}\le x_{st}+x_{tu}xsu​≤xst​+xtu​ whenever s<t<us<t<us<t<u;
  • S₂: the joint distributions of (xs+1,t+1)(x_{s+1,t+1})(xs+1,t+1​) are the same as those of (xst)(x_{st})(xst​);
  • S₃: gt=E(x0t)g_t=E(x_{0t})gt​=E(x0t​) is finite for every t≥1t\ge1t≥1 and gt≥−Atg_t\ge -Atgt​≥−At for some constant AAA;
  • S₃′: E(x01+)<∞E(x_{01}^+)<\inftyE(x01+​)<∞, where x+=max⁡(x,0)x^+=\max(x,0)x+=max(x,0).

A family of real random variables satisfying S₁, S₂ and S₃ is a subadditive process. Kingman's Theorem 1 (the goal of the first mission of this series) says that for a subadditive process x0t/tx_{0t}/tx0t​/t converges almost surely and in mean to a finite random variable ξ\xiξ with E(ξ)=γ=inf⁡t≥1gt/tE(\xi)=\gamma=\inf_{t\ge1}g_t/tE(ξ)=γ=inft≥1​gt​/t.

A Banach algebra B\mathfrak BB is a complete normed algebra over R\mathbb RR or C\mathbb CC whose norm satisfies ∥AB∥≤∥A∥ ∥B∥\|AB\|\le\|A\|\,\|B\|∥AB∥≤∥A∥∥B∥. A sequence (Yn)n≥1(Y_n)_{n\ge1}(Yn​)n≥1​ of B\mathfrak BB-valued random elements is stationary if (Yn+1)n≥1(Y_{n+1})_{n\ge1}(Yn+1​)n≥1​ and (Yn)n≥1(Y_n)_{n\ge1}(Yn​)n≥1​ have the same joint law. The log-norm process is

xst=log⁡∥Ys+1Ys+2⋯Yt∥∈[−∞,∞),s<t,x_{st}=\log\|Y_{s+1}Y_{s+2}\cdots Y_t\|\in[-\infty,\infty),\qquad s<t,xst​=log∥Ys+1​Ys+2​⋯Yt​∥∈[−∞,∞),s<t,

with log⁡0=−∞\log 0=-\inftylog0=−∞. Expectations of [−∞,∞)[-\infty,\infty)[−∞,∞)-valued variables are extended expectations E(f)=∫f+ dP−∫f− dPE(f)=\int f^+\,dP-\int f^-\,dPE(f)=∫f+dP−∫f−dP, defined when ∫f+ dP<∞\int f^+\,dP<\infty∫f+dP<∞ and possibly equal to −∞-\infty−∞.

Formalization targets

Goal: Theorem 6 (p. 893)

If (Yn)(Y_n)(Yn​) is a stationary sequence in a real or complex Banach algebra and E{(log⁡∥Y1∥)+}<∞E\{(\log\|Y_1\|)^+\}<\inftyE{(log∥Y1​∥)+}<∞, then

ξ=lim⁡n→∞n−1log⁡∥Y1Y2⋯Yn∥\xi=\lim_{n\to\infty}n^{-1}\log\|Y_1Y_2\cdots Y_n\|ξ=n→∞lim​n−1log∥Y1​Y2​⋯Yn​∥

exists in −∞≤ξ<∞-\infty\le\xi<\infty−∞≤ξ<∞ with probability one, and

E(ξ)=lim⁡n→∞n−1E{log⁡∥Y1Y2⋯Yn∥}.E(\xi)=\lim_{n\to\infty}n^{-1}E\{\log\|Y_1Y_2\cdots Y_n\|\}.E(ξ)=n→∞lim​n−1E{log∥Y1​Y2​⋯Yn​∥}.

The goal fixes no constant and no ergodicity assumption: ξ\xiξ is in general a non-degenerate random variable.

Milestones

  1. (1.2.7), p. 885: under S₁, S₂ and S₃′, E(xst+)<∞E(x_{st}^+)<\inftyE(xst+​)<∞ for all s<ts<ts<t.
  2. Proof of Theorem 2, p. 886: the truncation xst(N)=max⁡(xst,−N(t−s))x^{(N)}_{st}=\max(x_{st},-N(t-s))xst(N)​=max(xst​,−N(t−s)) is a subadditive process for every positive integer NNN.
  3. Theorem 2, p. 885: if xxx satisfies S₁, S₂ and S₃′ but not S₃, then ξ=lim⁡x0t/t\xi=\lim x_{0t}/tξ=limx0t​/t exists with probability one in [−∞,∞)[-\infty,\infty)[−∞,∞) and E(ξ)=−∞E(\xi)=-\inftyE(ξ)=−∞.
  4. Proof of Theorem 6, p. 893: the log-norm process satisfies S₁, S₂ and S₃′.

Significance

Theorem 6 defines a stochastic spectral radius: if every YnY_nYn​ equals a fixed element yyy, then eξe^\xieξ is the spectral radius of yyy by Gelfand's formula, and for independent YnY_nYn​ with common law π\piπ the limit is a constant ρ(π)\rho(\pi)ρ(π) depending only on π\piπ. For k×kk\times kk×k matrices the theorem reduces to the Furstenberg–Kesten theorem. Theorem 2, the extension of the subadditive ergodic theorem from S₃ to S₃′, is the form needed whenever a process can have mean growth rate −∞-\infty−∞, as happens for products that can vanish or contract superlinearly; it is used well beyond random products.

All results here are proved on paper (Kingman 1973, building on his 1968 paper). None of them is machine-checked: Mathlib has no subadditive ergodic theorem, no Furstenberg–Kesten theorem and no random-product limit in normed algebras. The platform poses an ergodic, constant-limit form of Kingman's theorem (PalmQueueing.Ergodic.kingman_subadditive, open); this mission's Theorem 2 is a different statement (non-ergodic, conclusion E(ξ)=−∞E(\xi)=-\inftyE(ξ)=−∞ under failure of S₃). A complete development would give the first formal proof of the Furstenberg–Kesten limit, in the generality of Banach algebras.

Difficulty

Theorem 6 is short given Theorems 1 and 2, but the obvious one-line reduction to Theorem 1 fails in two places. First, the log-norm process can take the value −∞-\infty−∞ and its means gtg_tgt​ can be −∞-\infty−∞ or decrease superlinearly, so condition S₃ fails and Theorem 1 does not apply; the case E(ξ)=−∞E(\xi)=-\inftyE(ξ)=−∞ is a separate theorem (Theorem 2), whose proof must exchange a limit in ttt with a limit in an auxiliary parameter. Second, stationarity of the log-norm process (S₂) is a statement about joint laws on a path space; in a non-separable Banach algebra, multiplication need not be measurable for the product σ\sigmaσ-algebra on B×B\mathfrak B\times\mathfrak BB×B, so it is not automatic that the law of (Yn)(Y_n)(Yn​) determines the joint law of the products Ys+1⋯YtY_{s+1}\cdots Y_tYs+1​⋯Yt​. The main dependency, Theorem 1 itself, is the subject of a separate mission and is not restated here.

Formalization scope

The Lean development fixes these conventions:

  • Families are functions x : ℕ → ℕ → Ω → β; only pairs s<ts<ts<t enter any condition. S₁ is required almost surely for each triple (the weaker hypothesis); the log-norm milestone proves it at every sample point.
  • S₂ and stationarity are equalities of laws of the whole path (Measure.map) on the product σ\sigmaσ-algebra, not equality of one-dimensional marginals.
  • S₃′ and all positive parts are lower Lebesgue integrals; expectations that may be −∞-\infty−∞ are computed as ∫f+−∫f−\int f^+ - \int f^-∫f+−∫f− in EReal, never as Bochner integrals (which return 000 for non-integrable functions).
  • log⁡∥⋅∥\log\|\cdot\|log∥⋅∥ is ENNReal.log of the norm, so log⁡∥0∥=−∞\log\|0\|=-\inftylog∥0∥=−∞; Real.log 0 = 0 would replace a vanishing product's growth rate −∞-\infty−∞ by 000, and is ruled out.
  • B\mathfrak BB is a complete unital NormedRing with NormedAlgebra 𝕜 𝔅, RCLike 𝕜. Each YnY_nYn​ is strongly measurable; B\mathfrak BB is not assumed separable.
  • Limits are Filter.atTop on ℕ in the topology of EReal; the conclusions assert ξ<∞\xi<\inftyξ<∞ almost surely, E(ξ+)<∞E(\xi^+)<\inftyE(ξ+)<∞, and, for (2.3.5), both the existence of the limit of means and its value.

A formalization that replaces the extended logarithm by Real.log, or the extended expectation by a Bochner integral, makes the statement false or trivially different, and is excluded.

Reusable infrastructure: extended expectations of EReal-valued random variables, joint-law stationarity of sequences and two-parameter families, and the truncation lemma for S₃′ processes. Contributions toward Theorem 1 (mission 1 of this series), toward measurability of products of strongly measurable random elements, and toward the milestones in any order are welcome.

Selected references

  • J. F. C. Kingman, Subadditive ergodic theory, Ann. Probab. 1(6):883–899, 1973. https://doi.org/10.1214/aop/1176996798
  • J. F. C. Kingman, The ergodic theory of subadditive stochastic processes, J. Roy. Statist. Soc. Ser. B 30:499–510, 1968. https://doi.org/10.1111/j.2517-6161.1968.tb00749.x
  • H. Furstenberg and H. Kesten, Products of random matrices, Ann. Math. Statist. 31:457–469, 1960. https://doi.org/10.1214/aoms/1177705909
8 thms2 active usersReviewed
Dynamical SystemsOperations ResearchProbability·Captain: mikedeng1

Subadditive Ergodic Theory 4: Furstenberg–Kesten — for Stationary Positive Random Matrices, n⁻¹ log [Y₁⋯Y_n]_ij Converges, Independently of i and jResearch Paper

Products of random matrices

Many systems evolve by repeated multiplication by a random linear map: the state of a linear system with randomly varying coefficients, population vectors in a random environment (Leslie models whose rates change from year to year), the transfer matrices of a disordered one-dimensional medium, and the transition operators of a Markov chain in a random environment. In each case the object of interest is the product Xn=Y1Y2⋯YnX_n = Y_1 Y_2 \cdots Y_nXn​=Y1​Y2​⋯Yn​ of random matrices and its growth as n→∞n\to\inftyn→∞.

The basic answer is due to Furstenberg and Kesten (Products of random matrices, Ann. Math. Statist. 31 (1960)): under a logarithmic moment condition and stationarity, n−1log⁡n^{-1}\logn−1log of the size of XnX_nXn​ converges. Their proof was a substantial piece of analysis. In his 1973 IMS Special Invited Paper (Kingman, Subadditive ergodic theory, Ann. Probab. 1 (1973)), J. F. C. Kingman showed that for matrices with strictly positive entries the result is a short corollary of his subadditive ergodic theorem (Theorem 1 of that paper, 1968). This mission formalizes that application: Theorem 5 of the 1973 paper, §2.2, pp. 891–892.

Timeline:

  • 1960: Furstenberg and Kesten prove convergence of n−1log⁡∥Xn∥n^{-1}\log\|X_n\|n−1log∥Xn​∥ and, for positive matrices, of n−1log⁡[Xn]ijn^{-1}\log[X_n]_{ij}n−1log[Xn​]ij​.
  • 1968: Kingman proves the subadditive ergodic theorem (J. Roy. Statist. Soc. B 30).
  • 1973: Kingman's survey deduces the positive-matrix theorem (Theorem 5) and the general Banach-algebra version (Theorem 6) from it.

Setting

Let (Ω,F,P)(\Omega,\mathcal F,P)(Ω,F,P) be a probability space, k≥1k\ge1k≥1, and let Y1,Y2,…Y_1, Y_2,\dotsY1​,Y2​,… be random k×kk\times kk×k real matrices. Write [A]ij[A]_{ij}[A]ij​ for the (i,j)(i,j)(i,j)th entry of a matrix AAA, and

Xn=Y1Y2⋯Yn(2.2.1),X_n = Y_1 Y_2\cdots Y_n \qquad (2.2.1),Xn​=Y1​Y2​⋯Yn​(2.2.1),

the product taken left to right. The sequence (Yn)(Y_n)(Yn​) is stationary if the joint law of (Y2,Y3,… )(Y_2, Y_3, \dots)(Y2​,Y3​,…) equals the joint law of (Y1,Y2,… )(Y_1, Y_2, \dots)(Y1​,Y2​,…); this is a statement about all finite-dimensional distributions at once, and it includes the case of independent identically distributed matrices.

The proof works with the diagonal process

zst=[Ys+1Ys+2⋯Yt]11,xst=−log⁡zst(s<t),z_{st} = [Y_{s+1}Y_{s+2}\cdots Y_t]_{11},\qquad x_{st} = -\log z_{st}\qquad (s<t),zst​=[Ys+1​Ys+2​⋯Yt​]11​,xst​=−logzst​(s<t),

and with the ℓ1\ell_1ℓ1​-norm ∥A∥=max⁡i∑j∣[A]ij∣\|A\| = \max_i \sum_j |[A]_{ij}|∥A∥=maxi​∑j​∣[A]ij​∣. A family (xst)s<t(x_{st})_{s<t}(xst​)s<t​ is a subadditive process (§1.1) if S₁: xsu≤xst+xtux_{su}\le x_{st}+x_{tu}xsu​≤xst​+xtu​ for s<t<us<t<us<t<u; S₂: the joint distributions of (xs+1,t+1)(x_{s+1,t+1})(xs+1,t+1​) equal those of (xst)(x_{st})(xst​); S₃: gt=E(x0t)g_t=E(x_{0t})gt​=E(x0t​) exists and gt≥−Atg_t\ge -Atgt​≥−At for some constant AAA.

Formalization targets

Goal: Theorem 5

Suppose the elements of the matrices YnY_nYn​ are strictly positive, E∣log⁡[Yn]ij∣<∞E|\log[Y_n]_{ij}|<\inftyE∣log[Yn​]ij​∣<∞ for every nnn and every i,ji,ji,j, and (Yn)(Y_n)(Yn​) is stationary. Then there is one finite random variable λ\lambdaλ such that for every (i,j)(i,j)(i,j)

λ=lim⁡n→∞n−1log⁡[Xn]ij(2.2.2)\lambda = \lim_{n\to\infty} n^{-1}\log [X_n]_{ij} \qquad (2.2.2)λ=n→∞lim​n−1log[Xn​]ij​(2.2.2)

with probability one and in mean. The limit is random in general (it is constant when (Yn)(Y_n)(Yn​) is ergodic); the theorem asserts its existence, its finiteness and its independence of (i,j)(i,j)(i,j), and nothing about its value.

Milestones, in the order of the paper's proof

  1. (2.3.1): [AB]11≥[A]11[B]11[AB]_{11}\ge[A]_{11}[B]_{11}[AB]11​≥[A]11​[B]11​ for matrices with strictly positive entries.
  2. xst=−log⁡zstx_{st}=-\log z_{st}xst​=−logzst​ satisfies S₁ and S₂, and each xstx_{st}xst​ has finite expectation gt−sg_{t-s}gt−s​.
  3. E{log⁡∥Y1∥}<∞E\{\log\|Y_1\|\}<\inftyE{log∥Y1​∥}<∞ and gn/n≥−E{log⁡∥Y1∥}g_n/n\ge -E\{\log\|Y_1\|\}gn​/n≥−E{log∥Y1​∥} for all n≥1n\ge1n≥1, so S₃ holds.
  4. The limit (2.2.2) exists, with probability one and in mean, for i=j=1i=j=1i=j=1.
  5. (2.2.3): for every (i,j)(i,j)(i,j), P{lim inf⁡n−1log⁡[Xn]ij≥λ}=1P\{\liminf n^{-1}\log[X_n]_{ij}\ge\lambda\}=1P{liminfn−1log[Xn​]ij​≥λ}=1.
  6. For every (i,j)(i,j)(i,j), P{lim sup⁡n−1log⁡[Xn]ij≤λ}=1P\{\limsup n^{-1}\log[X_n]_{ij}\le\lambda\}=1P{limsupn−1log[Xn​]ij​≤λ}=1.

Significance

The limit λ\lambdaλ is the top Lyapunov exponent of the random product: it is the almost-sure exponential growth rate of every entry, and hence of every norm, of XnX_nXn​. It governs the stability of random linear recursions vn=vn−1Ynv_{n}=v_{n-1}Y_nvn​=vn−1​Yn​, the long-run growth rate of populations in random environments, and localization in one-dimensional disordered systems. Theorem 5 is the existence statement on which all of these quantitative questions rest.

The theorem has been proved since 1960, and Kingman's derivation is a classical model application of subadditive ergodic theory. To our knowledge it has no machine-checked proof: Mathlib has neither Kingman's subadditive ergodic theorem nor any limit theorem for random matrix products. This mission produces a formal statement of the result together with the formal decomposition of the proof into the steps Kingman writes down; its milestone 4 is exactly where the subadditive ergodic theorem (the goal of the companion mission Subadditive Ergodic Theory 1) is applied.

Difficulty

Milestones 1–3 are deterministic matrix inequalities plus integrability bookkeeping; the substance is elsewhere. First, milestone 4 needs the full subadditive ergodic theorem, almost-sure and in mean, for a non-ergodic stationary process: the classical Birkhoff theorem does not apply, because log⁡[Xn]11\log[X_n]_{11}log[Xn​]11​ is not a sum of stationary increments. Second, passing from the diagonal entry to all entries requires controlling n−1log⁡[Yn]1jn^{-1}\log[Y_n]_{1j}n−1log[Yn​]1j​ along a stationary sequence with only a first-moment hypothesis, and transporting an almost-sure statement about Xn′=Y2⋯Yn+1X_n'=Y_2\cdots Y_{n+1}Xn′​=Y2​⋯Yn+1​ back to XnX_nXn​ by stationarity, where the limit λ\lambdaλ is itself random. The natural shortcut — treating λ\lambdaλ as a constant — is only valid under ergodicity, which is not assumed.

Formalization scope

  • Matrices are Matrix (Fin k) (Fin k) ℝ with NeZero k; the paper's index 111 is 0 : Fin k. The sequence is Y : ℕ → Ω → Matrix …, read only for n≥1n\ge1n≥1; Y 0 plays no role.
  • Products are ordered: Ys+1⋯YtY_{s+1}\cdots Y_tYs+1​⋯Yt​ is the List.prod of [Y (s+1), …, Y t]; X0X_0X0​ is the identity.
  • Stationarity is equality of the laws of (Yn+2)n≥0(Y_{n+2})_{n\ge0}(Yn+2​)n≥0​ and (Yn+1)n≥0(Y_{n+1})_{n\ge0}(Yn+1​)n≥0​ on ℕ → Fin k → Fin k → ℝ with the product σ-algebra. Independence is not assumed.
  • Positivity holds for every outcome; "their logarithms have finite expectations" is integrability of every log⁡[Yn]ij\log[Y_n]_{ij}log[Yn​]ij​, n≥1n\ge1n≥1.
  • "Finite limit" is a real-valued lam : Ω → ℝ; "in mean" is E∣n−1log⁡[Xn]ij−λ∣→0E|n^{-1}\log[X_n]_{ij}-\lambda|\to0E∣n−1log[Xn​]ij​−λ∣→0 with λ\lambdaλ integrable; time is n∈Nn\in\mathbb Nn∈N with Filter.atTop. One lam serves all (i,j)(i,j)(i,j).
  • Lim inf and lim sup inequalities are stated with ε\varepsilonε: almost surely, for every ε>0\varepsilon>0ε>0, eventually n−1log⁡[Xn]ij≥λ−εn^{-1}\log[X_n]_{ij}\ge\lambda-\varepsilonn−1log[Xn​]ij​≥λ−ε (respectively ≤λ+ε\le\lambda+\varepsilon≤λ+ε), which avoids the junk value of a real liminf on unbounded sequences.
  • Real.log 0 = 0 in Lean; the statements apply log only to entries that are strictly positive under the hypotheses, so no junk value enters. Dropping the positivity hypothesis would change the theorem, and is not an acceptable shortcut.
  • The S₁/S₂ vocabulary of §1.1 comes from the group's shared process module; this mission defines gtg_tgt​ locally. The general subadditive ergodic theorem is not restated here, and milestone 4 is the object-specific statement the paper writes.

Welcome contributions: proofs of the matrix inequalities, the integrability and stationarity transfer lemmas, a formal subadditive ergodic theorem (shared with the companion mission).

Selected references

  • J. F. C. Kingman, Subadditive ergodic theory, Ann. Probab. 1(6):883–899, 1973. https://doi.org/10.1214/aop/1176996798
  • H. Furstenberg and H. Kesten, Products of random matrices, Ann. Math. Statist. 31(2):457–469, 1960. https://doi.org/10.1214/aoms/1177705909
  • J. F. C. Kingman, The ergodic theory of subadditive stochastic processes, J. Roy. Statist. Soc. Ser. B 30(3):499–510, 1968. https://doi.org/10.1111/j.2517-6161.1968.tb00749.x
9 thms2 active usersReviewed
Linear OptimizationOperations ResearchOptimization+1·Captain: mikedeng1

On Adaptive-Step Primal-Dual Interior-Point Algorithms for Linear Programming 4: For a Random Subspace, ‖Pq‖⁻∞ ≤ (log n/n)‖r‖² with Probability Tending to OneResearch Paper

Motivation

Primal–dual interior point methods follow a path of strictly feasible solutions to a linear program. Their worst case iteration bounds come from controlling a term that is quadratic in each search step. Mizuno, Todd, and Ye asked whether that term is typically much smaller than its worst case bound under a model in which a certain subspace is randomly oriented. Theorem 5 in their technical report gives a probability bound for the negative part of that term. It is a statement about one randomly oriented subspace and a fixed input vector, rather than a stochastic model for an entire algorithm run. The authors explicitly note that assigning the same random subspace model independently at successive iterations would be inconsistent with the algorithm's evolving state. Mizuno, Todd, and Ye, §6

Setting

Fix a dimension nnn, an integer ddd with 0≤d≤n0\le d\le n0≤d≤n, and a vector r∈Rnr\in\mathbb R^nr∈Rn. Draw a random ddd-dimensional subspace UUU from the distribution invariant under orthogonal transformations. Let ppp be the Euclidean orthogonal projection of rrr onto UUU, and put q=r−pq=r-pq=r−p, its projection onto U⊥U^\perpU⊥. The matrix P=diag⁡(p)P=\operatorname{diag}(p)P=diag(p) turns the vector qqq into the coordinatewise product Pq=(pjqj)j=1nPq=(p_jq_j)_{j=1}^nPq=(pj​qj​)j=1n​.

For a coordinate vector zzz, let z−=(min⁡{zj,0})j=1nz^-=(\min\{z_j,0\})_{j=1}^nz−=(min{zj​,0})j=1n​ and ∥z∥∞−=∥z−∥∞\|z\|^-_\infty=\|z^-\|_\infty∥z∥∞−​=∥z−∥∞​. Thus ∥Pq∥∞−\|Pq\|^-_\infty∥Pq∥∞−​ records the magnitude of the largest negative coordinate of PqPqPq. An unsubscripted vector norm is always the Euclidean ℓ2\ell_2ℓ2​ norm. These definitions follow the report's notation on printed pages 2 and 4. Mizuno, Todd, and Ye, §§1–2

The formal model samples an (n−d)×n(n-d)\times n(n−d)×n matrix GGG with independent standard normal entries and sets U=ker⁡GU=\ker GU=kerG. The report itself gives this construction as an example of the orthogonally invariant law. With probability one, this null space has dimension ddd. The construction covers the endpoint cases d=0d=0d=0 and d=nd=nd=n as well: the projection product is then zero. This probabilistic model has no linear programming data in its statement. The optimization setting explains why the quantity matters, while the result depends only on Euclidean projection geometry. Mizuno, Todd, and Ye, §6

Formalization targets

Theorem 5

For arbitrary choices rn∈Rnr_n\in\mathbb R^nrn​∈Rn and dn≤nd_n\le ndn​≤n at each dimension, the central target is

Pr⁡{∥Pnqn∥∞−≤log⁡nn∥rn∥22}⟶1(n⟶∞).\Pr\left\{\|P_nq_n\|^-_\infty\le \frac{\log n}{n}\|r_n\|_2^2\right\} \longrightarrow 1\qquad(n\longrightarrow\infty).Pr{∥Pn​qn​∥∞−​≤nlogn​∥rn​∥22​}⟶1(n⟶∞).

The logarithm is natural. The theorem asks for the exact coefficient shown in the report, rather than only an asymptotic order. The choice of rnr_nrn​ and dnd_ndn​ may change with nnn; the result does not require a common probability space for all dimensions. Mizuno, Todd, and Ye, Theorem 5, printed p. 13

Source milestones

The mission includes Lemma 6, which identifies a beta distributed radial coordinate and a uniform spherical direction for a projected vector; the componentwise identities and inequality (18)–(19); the Gaussian norm limit (20); the Gaussian coordinate maximum limit cited in the proof; and Lemma 7, which bounds the sup norm of a rotated uniform spherical direction by 3log⁡n/n\sqrt{3\log n/n}3logn/n​ with probability tending to one. Their statements, constants, and order follow printed pages 14–15 of the report. Mizuno, Todd, and Ye, §6

Significance

The result gives a precise high probability bound for the negative coordinates of the projection product. In the report this product represents the second order term of a primal–dual search direction, and a smaller value permits a larger admissible step in the relevant neighborhood analysis. The theorem therefore supplies a mathematically definite part of the paper's discussion of anticipated improved behavior. It does not by itself prove a typical iteration count: the paper does not provide a consistent random model for the sequence of subspaces visited by the algorithm. Mizuno, Todd, and Ye, §§2, 6–7

The report proves Theorem 5 and the two numbered lemmas on paper. The formalization work is to provide machine checked proofs of the random subspace representation, the beta and spherical laws, the finite dimensional Gaussian limits, and their connection to the projection bound. These results are reusable in other questions about random projections and coordinatewise estimates. The statements in this mission are open formalization targets; compilation of a statement with a proof placeholder does not count as a machine checked proof.

Difficulty

A direct norm bound on ppp and qqq loses the coordinate information needed for the factor log⁡n/n\log n/nlogn/n. The difficult part is that the desired bound concerns the most negative coordinate of a product of two dependent projections, while the distribution is specified through a random subspace. The paper's deterministic identity (18)–(19) relates this product to an angular coordinate. The remaining probabilistic statements must control the largest coordinate of a uniformly distributed spherical vector, including the numerical constant in Lemma 7. The laws of the radial and angular coordinates also need a sound measurable construction; simply writing a mapped measure without checking the map would not establish the claimed distributions.

Formalization scope

Vectors are EuclideanSpace ℝ (Fin n), so ∥r∥\|r\|∥r∥ is the ℓ2\ell_2ℓ2​ norm. Coordinate sup norms are separate definitions. A complete development needs finite dimensional inner product geometry, orthogonal projections, Gaussian product measures, beta measures, the uniform spherical law, and limits of real probabilities. The spherical law is encoded as the direction of a standard Gaussian vector. The Gaussian matrix construction fixes the invariant subspace distribution and must be connected to the stated ddd-dimensional law almost surely.

Lemma 6 concerns d,m≥1d,m\ge1d,m≥1 and n≥2n\ge2n≥2, where the beta parameters and the spherical direction are nondegenerate. Its angular direction is assigned zero at the zero coordinate, which has probability zero in this regime; the claimed decomposition and unit norm hold almost surely. Theorem 5 retains d=0d=0d=0, d=nd=nd=n, and r=0r=0r=0. Lemma 7 is stated only for frames in dimensions at least two; finitely many smaller dimensions are assigned probability one in its limit expression. Equation (20) keeps the report's condition ε>0\varepsilon>0ε>0. All limits are probabilities tending to one, never probability one at every finite nnn.

Contributions should preserve the source's constants and all three claims of Lemma 6. A proof of the beta law alone, or a bound for a single fixed direction, does not close the corresponding target. The invariant random subspace and projection model, the Gaussian and spherical distribution facts, and the coordinate estimates are each useful independently of this mission.

Selected references

  • Shinji Mizuno, Michael J. Todd, and Yinyu Ye, On Adaptive-Step Primal-Dual Interior-Point Algorithms for Linear Programming, Cornell ORIE Technical Report No. 944, 1990, revised 1991; published in Mathematics of Operations Research 18(4), 1993. DOI
  • Sidney I. Resnick, Extreme Values, Regular Variation, and Point Processes, Springer, 1987, pp. 42 and 71, cited in the report for the Gaussian maximum estimate. DOI
7 thms2 active usersReviewed
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
14 thms2 active usersReviewed
Operations ResearchProbabilityStatistics·Captain: mikedeng1

The Risk of Expected Utility Under Parameter Uncertainty I: Closed-Form Out-of-Sample Utility Variance of the Shrinkage Mean-Variance PortfolioResearch Paper

Why out-of-sample utility risk matters

A portfolio chosen from historical returns can look attractive in the data used to construct it and deliver a different result when evaluated under the population return distribution. The gap is driven by estimation error in both the mean return and covariance matrix. A mean of future utility values describes average performance, but it does not describe how much that utility varies across possible estimation samples. Lassance, Martín-Utrera and Simaan study this variation for a portfolio that blends an estimated mean-variance choice with an estimated global-minimum-variance choice. Their closed-form variance makes the sampling risk of that blend an explicit function of market and sample parameters. The source for this mission is the authors’ SSRN manuscript, version dated August 18, 2023, including its Internet Appendix; appendix pages are cited as IA pages.

The market and the estimated portfolio

There are NNN risky stocks. Their excess-return vector has population mean μ∈RN\mu\in\mathbb R^Nμ∈RN and positive-definite population covariance Σ∈RN×N\Sigma\in\mathbb R^{N\times N}Σ∈RN×N. The investor has risk aversion γ>0\gamma>0γ>0. A portfolio is a vector of weights www whose entries sum to one. Its population mean-variance utility is

U(w)=w⊤μ−γ2w⊤Σw.U(w)=w^\top\mu-\frac{\gamma}{2}w^\top\Sigma w.U(w)=w⊤μ−2γ​w⊤Σw.

Write eee for the vector of ones. The global-minimum-variance portfolio and its variance are wg=Σ−1e(e⊤Σ−1e)−1w_g=\Sigma^{-1}e(e^\top\Sigma^{-1}e)^{-1}wg​=Σ−1e(e⊤Σ−1e)−1 and σg2=(e⊤Σ−1e)−1\sigma_g^2=(e^\top\Sigma^{-1}e)^{-1}σg2​=(e⊤Σ−1e)−1. Its mean is μg=μ⊤Σ−1e σg2\mu_g=\mu^\top\Sigma^{-1}e\,\sigma_g^2μg​=μ⊤Σ−1eσg2​. The population matrix B=Σ−1(I−ewg⊤)B=\Sigma^{-1}(I-ew_g^\top)B=Σ−1(I−ewg⊤​) maps the mean vector to a zero-cost portfolio. The variance of that portfolio is ψ2=μ⊤Σ−1μ−μg2/σg2\psi^2=\mu^\top\Sigma^{-1}\mu-\mu_g^2/\sigma_g^2ψ2=μ⊤Σ−1μ−μg2​/σg2​. These quantities are computed from μ\muμ and Σ\SigmaΣ; they are not independent inputs. These definitions are equations (3)–(7) of the manuscript.

The investor observes TTT independent return vectors r1,…,rTr_1,\ldots,r_Tr1​,…,rT​, each with multivariate Gaussian law N(μ,Σ)\mathcal N(\mu,\Sigma)N(μ,Σ). The sample mean is μ^=T−1∑trt\hat\mu=T^{-1}\sum_t r_tμ^​=T−1∑t​rt​, and the sample covariance is Σ^=T−1∑t(rt−μ^)(rt−μ^)⊤\hat\Sigma=T^{-1}\sum_t(r_t-\hat\mu)(r_t-\hat\mu)^\topΣ^=T−1∑t​(rt​−μ^​)(rt​−μ^​)⊤. Replacing the population parameters in wgw_gwg​ and BBB by these estimates gives the sample GMV portfolio w^g\hat w_gw^g​ and the sample zero-cost portfolio w^z=B^μ^\hat w_z=\hat B\hat\muw^z​=B^μ^​. The estimated mean-variance portfolio is w^⋆=w^g+γ−1w^z\hat w^\star=\hat w_g+\gamma^{-1}\hat w_zw^⋆=w^g​+γ−1w^z​. At shrinkage intensity κ∈[0,1]\kappa\in[0,1]κ∈[0,1], the portfolio under study is w^⋆(κ)=(1−κ)w^g+κw^⋆\hat w^\star(\kappa)=(1-\kappa)\hat w_g+\kappa\hat w^\starw^⋆(κ)=(1−κ)w^g​+κw^⋆. Its out-of-sample utility, U(w^⋆(κ))U(\hat w^\star(\kappa))U(w^⋆(κ)), is evaluated using population μ\muμ and Σ\SigmaΣ. It is random because the weights depend on the sample. These choices are fixed by equations (9)–(12) and Assumption 2 of the manuscript.

Formalization targets

The goal is Proposition 1, equations (13)–(19). Under N≥2N\ge2N≥2 and T>N+7T>N+7T>N+7, it asserts that the utility has a finite second moment and that

V[U(w^⋆(κ))]=V[U(w^g)]+Δ(κ),Δ(κ)=a1κ4+a2κ3+a3κ2+a4κ.\mathbb V[U(\hat w^\star(\kappa))] =\mathbb V[U(\hat w_g)]+\Delta(\kappa),\qquad \Delta(\kappa)=a_1\kappa^4+a_2\kappa^3+a_3\kappa^2+a_4\kappa.V[U(w^⋆(κ))]=V[U(w^g​)]+Δ(κ),Δ(κ)=a1​κ4+a2​κ3+a3​κ2+a4​κ.

The coefficients a1,…,a4a_1,\ldots,a_4a1​,…,a4​ and V[U(w^g)]\mathbb V[U(\hat w_g)]V[U(w^g​)] are the exact rational expressions in T,N,γ,σg2,ψ2T,N,\gamma,\sigma_g^2,\psi^2T,N,γ,σg2​,ψ2 on pp. 14–15 of the manuscript. In particular, the result covers every κ∈[0,1]\kappa\in[0,1]κ∈[0,1], including the sample GMV portfolio at κ=0\kappa=0κ=0 and the sample mean-variance portfolio at κ=1\kappa=1κ=1.

The milestones follow the quantities named in the authors’ proof, Section IA.10. Equation (IA43) gives the covariance matrix of the random weights, and (IA44) gives the variance of their population mean return. The jointly distributed mean-return and return-variance pair in (IA45)–(IA48) supplies the setting for two auxiliary moment identities, (IA53) and (IA57). Equations (IA49), (IA59), and (IA60) give the first and second moments needed for return variance and mean return; (IA68) gives their covariance. All are statements from the Internet Appendix, pp. IA35–IA39.

What the result supplies

The expression tells an investor how the sampling risk of utility changes with the shrinkage intensity, sample size, stock count, risk aversion, and the two population variance parameters. The later comparison of variance-minimizing, mean-maximizing, and robustness-maximizing intensities uses this formula. Without Proposition 1, those comparisons have no explicit OOSU risk function to analyze. The result is already proved in the paper; this mission asks for its Lean proof and for reusable formal statements of the associated Gaussian portfolio and moment identities. No machine-checked proof of this paper’s proposition is included in the draft.

Where the difficulty lies

The sample covariance is random and its inverse appears in the estimated weights. Taking the variance of utility therefore involves inverse-covariance terms and moments beyond those needed for expected utility. The requirement T>N+7T>N+7T>N+7 is tied to existence of the fourth negative moment of a chi-squared variable in (IA57). A direct calculation that replaces random weights by their population counterparts loses the dependence on the estimation sample. A calculation from separate marginal laws also does not determine the covariance between mean return and return variance; the representation in (IA47)–(IA48) describes them jointly.

Formalization scope

The Lean market uses vectors Fin N → ℝ, matrices indexed by Fin N, and returns in EuclideanSpace ℝ (Fin N) to use Mathlib’s multivariate Gaussian law. The sample has Fin T observations on a probability space. Its covariance divisor is exactly TTT, as in (9). The standing assumptions are N≥2N\ge2N≥2, T>N+7T>N+7T>N+7, Σ≻0\Sigma\succ0Σ≻0, γ>0\gamma>0γ>0, and independent, identically distributed Gaussian returns. Every theorem about a variance or covariance explicitly asserts finite second moments; expectation statements explicitly assert integrability. The source’s finite-variance convention is thereby represented without Lean’s default value for a nonintegrable variance.

The left side of the goal is the probability-theory variance of utility under the sampling law. It is not defined by the closed formula. Likewise σg2\sigma_g^2σg2​, μg\mu_gμg​, and ψ2\psi^2ψ2 are computed from the market; independence is part of the sampling hypothesis. In the auxiliary representation, the chi-squared law is the squared norm of independent standard normals. The zero-degree cases and footnote 6’s N=2,3N=2,3N=2,3 rules are encoded explicitly. Mathlib’s matrix inverse and real division are total operations; their values on singular sample covariances or zero denominators do not alter the distributions because those events have probability zero under the stated assumptions. Contributions establishing the sample-covariance distribution, the joint representation, the negative moments, and the final variance identity are within scope and can support other Gaussian portfolio results.

Selected references

  • N. Lassance, A. Martín-Utrera, and M. Simaan, The Risk of Expected Utility under Parameter Uncertainty, authors’ SSRN manuscript dated August 18, 2023, subsequently in Management Science (2024). SSRN 3855546; DOI 10.1287/mnsc.2023.00178.
12 thms1 active userReviewed
ProbabilityStatistics·Captain: mikedeng1

Change-Point Detection in Dynamic Networks with Missing Links III: The Dyadic-Grid Matrix CUSUM Test Detects an Unknown Change Time Above Energy 4(1+ϵ)(6ω_n/T)^{1/2} + C log(4n log₂T/(α∧β))/√TResearch Paper

Detecting a change in a partially observed network

Many networks are recorded as a sequence of snapshots: contact networks in epidemiology, communication graphs, brain connectivity measured over time, trade or transport links. A basic statistical question is whether the law generating the snapshots changed at some point. Two features make the question hard in practice. The networks are often sparse, so each snapshot carries little information. And links are missing: a pair of vertices is observed only with some probability, so an absent edge may mean "no link" or "not sampled".

Enikeeva and Klopp (arXiv:2106.14470, Operations Research, 2025) give minimax bounds for this testing problem. They treat both a known change time (Theorems 1 and 2) and an unknown change time (Theorem 3). This mission formalizes the unknown-time case, where the test scans a dyadic grid of candidate times. Two companion missions formalize the known-time upper bound (Theorem 1) and the lower bound (Theorem 2).

Setting

There are nnn vertices and TTT time points. At time ttt the statistician observes a symmetric matrix Yt∈{0,1}n×nY^t\in\{0,1\}^{n\times n}Yt∈{0,1}n×n with zero diagonal, Yijt=ΩijtAijtY^t_{ij}=\Omega^t_{ij}A^t_{ij}Yijt​=Ωijt​Aijt​. Here AtA^tAt is the adjacency matrix of the network and Ωt\Omega^tΩt records which pairs were sampled. The entries YijtY^t_{ij}Yijt​, i<ji<ji<j, are independent over pairs and times, and

Yijt∼Bernoulli((Π⊙Θt)ij),Y^t_{ij}\sim\mathrm{Bernoulli}\big((\Pi\odot\Theta^t)_{ij}\big),Yijt​∼Bernoulli((Π⊙Θt)ij​),

where Θt∈[0,1]n×n\Theta^t\in[0,1]^{n\times n}Θt∈[0,1]n×n is the connection-probability matrix (symmetric, zero diagonal), Π\PiΠ is the sampling matrix (symmetric, entries in (0,1](0,1](0,1], unit diagonal), and ⊙\odot⊙ is the entrywise product.

The sparsity level ωn\omega_nωn​ bounds the expected observed degree: (Θ,Π)∈Sn(ωn)(\Theta,\Pi)\in\mathcal S_n(\omega_n)(Θ,Π)∈Sn​(ωn​) when ∥Π⊙Θ∥1,∞=max⁡j∑i∣(Π⊙Θ)ij∣≤ωn\|\Pi\odot\Theta\|_{1,\infty}=\max_j\sum_i|(\Pi\odot\Theta)_{ij}|\le\omega_n∥Π⊙Θ∥1,∞​=maxj​∑i​∣(Π⊙Θ)ij​∣≤ωn​.

Under the null hypothesis Θt=Θ0\Theta^t=\Theta^0Θt=Θ0 for all ttt. Under the alternative there is τ∈DT={1,…,T−1}\tau\in\mathcal D_T=\{1,\dots,T-1\}τ∈DT​={1,…,T−1} with Θt=Θ0\Theta^t=\Theta^0Θt=Θ0 for t≤τt\le\taut≤τ and Θt=Θ0+ΔΘτ\Theta^t=\Theta^0+\Delta\Theta^\tauΘt=Θ0+ΔΘτ for t>τt>\taut>τ. Both parameter pairs lie in Sn(ωn)\mathcal S_n(\omega_n)Sn​(ωn​), and the jump has energy at least RRR:

q(τ/T) ∥Π⊙ΔΘτ∥2→2≥R,q(x)=x(1−x),q(\tau/T)\,\|\Pi\odot\Delta\Theta^\tau\|_{2\to2}\ge R,\qquad q(x)=\sqrt{x(1-x)},q(τ/T)∥Π⊙ΔΘτ∥2→2​≥R,q(x)=x(1−x)​,

where ∥⋅∥2→2\|\cdot\|_{2\to2}∥⋅∥2→2​ is the spectral norm. A test ψ\psiψ maps the data to {0,1}\{0,1\}{0,1}. Its type I error α(ψ)\alpha(\psi)α(ψ) is the largest rejection probability over the null class. Its type II error β(ψ,R)\beta(\psi,R)β(ψ,R) is the largest acceptance probability over all τ∈DT\tau\in\mathcal D_Tτ∈DT​ and all alternatives of energy at least RRR.

The Matrix CUSUM at time ttt contrasts the averages before and after ttt:

ZT(t)=t(T−t)T(1t∑s=1tYs−1T−t∑s=t+1TYs),1≤t≤T−1.Z_T(t)=\sqrt{\frac{t(T-t)}{T}}\Big(\frac1t\sum_{s=1}^tY^s-\frac1{T-t}\sum_{s=t+1}^TY^s\Big),\qquad1\le t\le T-1.ZT​(t)=Tt(T−t)​​(t1​s=1∑t​Ys−T−t1​s=t+1∑T​Ys),1≤t≤T−1.

The dyadic grid is T={2k}∪{T−2k}\mathcal T=\{2^k\}\cup\{T-2^k\}T={2k}∪{T−2k}, 0≤k≤⌊log⁡2(T/2)⌋0\le k\le\lfloor\log_2(T/2)\rfloor0≤k≤⌊log2​(T/2)⌋. Fix ϵ∈(0,1/2]\epsilon\in(0,1/2]ϵ∈(0,1/2]. The test (14) of the paper rejects when

max⁡t∈T∥ZT(t)∥2→2>Hα,n,T=22(1+ϵ)ωn+Cϵlog⁡4nlog⁡2(T)α.\max_{t\in\mathcal T}\|Z_T(t)\|_{2\to2}>H_{\alpha,n,T}=2\sqrt2(1+\epsilon)\sqrt{\omega_n}+C_\epsilon\log\frac{4n\log_2(T)}{\alpha}.t∈Tmax​∥ZT​(t)∥2→2​>Hα,n,T​=22​(1+ϵ)ωn​​+Cϵ​logα4nlog2​(T)​.

Formalization targets

Goal: Theorem 3

For every ϵ∈(0,1/2]\epsilon\in(0,1/2]ϵ∈(0,1/2] there are constants Cϵ>0C_\epsilon>0Cϵ​>0 and CCC, depending only on ϵ\epsilonϵ, such that for all n≥1n\ge1n≥1, T≥2T\ge2T≥2, ωn≥0\omega_n\ge0ωn​≥0 and α,β∈(0,1)\alpha,\beta\in(0,1)α,β∈(0,1): if

R ≥ 4(1+ϵ)(6ωnT)1/2+CTlog⁡(4nlog⁡2(T)α∧β),R\ \ge\ 4(1+\epsilon)\Big(\frac{6\omega_n}{T}\Big)^{1/2}+\frac{C}{\sqrt T}\log\Big(\frac{4n\log_2(T)}{\alpha\wedge\beta}\Big),R ≥ 4(1+ϵ)(T6ωn​​)1/2+T​C​log(α∧β4nlog2​(T)​),

then the grid test with threshold Hα,n,TH_{\alpha,n,T}Hα,n,T​ has α(ψn,T)≤α\alpha(\psi_{n,T})\le\alphaα(ψn,T​)≤α and β(ψn,T,R)≤β\beta(\psi_{n,T},R)\le\betaβ(ψn,T​,R)≤β.

Milestones

  • the signal-plus-noise decomposition ZT(t)=−μTτ(t) Π⊙ΔΘτ+ξ(t)Z_T(t)=-\mu^\tau_T(t)\,\Pi\odot\Delta\Theta^\tau+\xi(t)ZT​(t)=−μTτ​(t)Π⊙ΔΘτ+ξ(t) and the maximum μTτ(τ)=T q(τ/T)\mu^\tau_T(\tau)=\sqrt T\,q(\tau/T)μTτ​(τ)=T​q(τ/T), display (7);
  • the grid facts T⊆DT\mathcal T\subseteq\mathcal D_TT⊆DT​ and ∣T∣≤2log⁡2T|\mathcal T|\le2\log_2T∣T∣≤2log2​T;
  • the grid captures signal: for every τ∈DT\tau\in\mathcal D_Tτ∈DT​ some t∈Tt\in\mathcal Tt∈T has μTτ(t)≥T q(τ/T)/3\mu^\tau_T(t)\ge\sqrt T\,q(\tau/T)/\sqrt3μTτ​(t)≥T​q(τ/T)/3​;
  • Proposition 11, the Bandeira–van Handel bound for symmetric random matrices with independent bounded entries;
  • Lemma 12, the noise bound for the CUSUM at a fixed time;
  • Lemma 5 (level) and Lemma 6 (power above 46(1+ϵ)(ωn/T)1/2+3CϵT(log⁡4nlog⁡2Tα+log⁡2nβ)4\sqrt6(1+\epsilon)(\omega_n/T)^{1/2}+\frac{\sqrt3C_\epsilon}{\sqrt T}(\log\frac{4n\log_2T}\alpha+\log\frac{2n}\beta)46​(1+ϵ)(ωn​/T)1/2+T​3​Cϵ​​(logα4nlog2​T​+logβ2n​)).

Significance

Theorem 3 shows that not knowing the change time costs at most a constant factor and a log⁡log⁡T\log\log TloglogT term in the detection energy. Together with the lower bound of Theorem 2, which is of order (ωn/T)1/2(\omega_n/T)^{1/2}(ωn​/T)1/2, this makes the grid test rate-optimal when ωn\omega_nωn​ grows at least polylogarithmically in nnn (Remark 3 of the paper). The statistic depends on the data only through spectral norms of O(log⁡T)O(\log T)O(logT) CUSUM matrices, so it is cheap to compute. The threshold needs only the degree bound ωn\omega_nωn​, which can be estimated from the observed degrees.

The paper's proof is complete on paper apart from one step noted below. No part of it is machine-checked. Formalizing it produces a checked finite model of Bernoulli network data with missing links, a reusable Matrix CUSUM, and a precise statement of a Bandeira–van Handel type bound for symmetric matrices with independent bounded entries. That bound is a standard tool in random-matrix statistics and is not yet available in Mathlib or on the platform.

Difficulty

The level of the test is a union bound over the grid combined with a high-probability bound on ∥ξ(t)∥2→2\|\xi(t)\|_{2\to2}∥ξ(t)∥2→2​ at a fixed time. The hard part is that bound, Lemma 12. A matrix Bernstein inequality gives a leading term σlog⁡(n/δ)\sigma\sqrt{\log(n/\delta)}σlog(n/δ)​, which is too large. The statement needs the sharp form 22(1+ϵ)σ+Cϵlog⁡(2n/δ)2\sqrt2(1+\epsilon)\sigma+C_\epsilon\log(2n/\delta)22​(1+ϵ)σ+Cϵ​log(2n/δ), where the variance proxy σ\sigmaσ enters without a logarithmic factor. Proposition 11 supplies this only for matrices whose entries are bounded by σ∗\sigma_*σ∗​. The entries of ξ(t)\xi(t)ξ(t) are sums over time and are only bounded by about log⁡(n/δ)\sqrt{\log(n/\delta)}log(n/δ)​ with high probability. The paper applies Proposition 11 "given the event" {∥ξ(t)∥∞≤σ∗}\{\|\xi(t)\|_\infty\le\sigma_*\}{∥ξ(t)∥∞​≤σ∗​}, but conditioning on that event destroys centring and independence, so a truncation argument is missing there.

The power analysis is elementary once Lemma 12 is available. Its one subtlety is that the change time ranges over all of DT\mathcal D_TDT​, while the test inspects only the grid.

Formalization scope

  • Data and probability. Only YYY is modelled; the latent At,ΩtA^t,\Omega^tAt,Ωt are integrated out. An observation is a Boolean function of a 0-based time index and of a pair i<ji<ji<j. Probabilities are finite sums of products of Bernoulli weights, so every test is measurable and no measure theory enters the model. Proposition 11 is the only measure-theoretic statement.
  • Classes. The sampling class carries the paper's standing assumptions Πii=1\Pi_{ii}=1Πii​=1, Πij>0\Pi_{ij}>0Πij​>0. The errors are real suprema of sets of probabilities; an empty alternative has type II error 000.
  • Spectral norm. ∥⋅∥2→2\|\cdot\|_{2\to2}∥⋅∥2→2​ is the published HighDimProb.RandomMatrices.matrixOpNorm.
  • Grid and test. ⌊log⁡2(T/2)⌋\lfloor\log_2(T/2)\rfloor⌊log2​(T/2)⌋ is Nat.log 2 (T / 2). "max⁡t∈T∥ZT(t)∥>H\max_{t\in\mathcal T}\|Z_T(t)\|>Hmaxt∈T​∥ZT​(t)∥>H" is "∃t∈T\exists t\in\mathcal T∃t∈T, ∥ZT(t)∥>H\|Z_T(t)\|>H∥ZT​(t)∥>H". The threshold uses the real log⁡2T\log_2Tlog2​T.
  • Constants. CϵC_\epsilonCϵ​ and CCC are quantified existentially before n,T,ωn,α,β,Rn,T,\omega_n,\alpha,\beta,Rn,T,ωn​,α,β,R. A version with the constants chosen after nnn or TTT would be trivial, because huge constants silence the test or empty the alternative. The goal does not assume Lemma 12's conclusion. Lemmas 5 and 6 take it as a hypothesis, and Lemma 12 states that it is satisfiable. The test ranges over all functions of the data, and the alternative over all τ∈DT\tau\in\mathcal D_Tτ∈DT​.
  • Disclosed additions and corrections. The theorems assume n≥1n\ge1n≥1, T≥2T\ge2T≥2 and ωn≥0\omega_n\ge0ωn​≥0, which the paper leaves implicit. Proposition 11 assumes m≥1m\ge1m≥1 and cϵ>0c_\epsilon>0cϵ​>0. Independence in Proposition 11 and Lemma 12 refers to the entries with i≤ji\le ji≤j (i<ji<ji<j) of a symmetric matrix. The grid statement is the inequality ∣T∣≤2log⁡2T|\mathcal T|\le2\log_2T∣T∣≤2log2​T: the printed equality ∣T∣=2+2⌊log⁡2(T/2)⌋|\mathcal T|=2+2\lfloor\log_2(T/2)\rfloor∣T∣=2+2⌊log2​(T/2)⌋ fails when the two halves overlap, as at T=4T=4T=4. Lemma 5 is stated with "≤α\le\alpha≤α", as its proof concludes, rather than the printed "less than α\alphaα". The grid-signal milestone is stated as an existence claim, because the printed choice τ/2≤t∗<τ\tau/2\le t^*<\tauτ/2≤t∗<τ has no solution at τ=1\tau=1τ=1.

Welcome contributions: a proof of Proposition 11, or of any sharp spectral-norm bound that implies it; a rigorous proof of Lemma 12, repairing the conditioning step; and the elementary grid lemmas.

Selected references

  • F. Enikeeva and O. Klopp, Change-point detection in dynamic networks with missing links, Operations Research, 2025; arXiv:2106.14470v2. https://arxiv.org/abs/2106.14470
  • A. S. Bandeira and R. van Handel, Sharp nonasymptotic bounds on the norm of random matrices with independent entries, Annals of Probability 44(4), 2016. https://doi.org/10.1214/15-AOP1025
  • H. Liu, C. Gao and R. J. Samworth, Minimax rates in sparse, high-dimensional change point detection, Annals of Statistics 49(2), 2021. https://doi.org/10.1214/20-AOS1994
12 thms1 active userReviewed
ProbabilityStatistics·Captain: mikedeng1

Change-Point Detection in Dynamic Networks with Missing Links II: At a Known Time the Matrix CUSUM Test Has Level α and Type II Error ≤ β Above Energy 4√2(1+ϵ)(ω_n/T)^{1/2} + C log(n/(α∧β))/√TResearch Paper

Motivation

Networks observed over time, such as communication graphs, contact networks and financial exposure graphs, often change structure abruptly. Change-point detection asks whether the law of the network changed during the observation window. In practice not every pair of nodes is observed at every time: links are missing because of sampling, privacy or measurement failure. Enikeeva and Klopp (arXiv:2106.14470, published in Operations Research, 2025) give the minimax detection boundary for this problem in a sparse inhomogeneous random graph model with missing links, for a change at a known time and at an unknown time.

This mission formalizes the upper bound at a known time (their Theorem 1): a test based on the spectral norm of a matrix-valued CUSUM statistic has level α\alphaα and type II error at most β\betaβ as soon as the change is a constant multiple of (ωn/T)1/2(\omega_n/T)^{1/2}(ωn​/T)1/2 plus a logarithmic term. The companion missions of this series formalize the matching lower bound (Theorem 2) and the unknown-time test (Theorem 3).

Setting

There are nnn vertices and TTT snapshots. At time ttt the network has a symmetric, zero-diagonal connection-probability matrix Θt∈[0,1]n×n\Theta^t\in[0,1]^{n\times n}Θt∈[0,1]n×n, and each pair i<ji<ji<j is sampled independently with probability Πij>0\Pi_{ij}>0Πij​>0, where the sampling matrix Π\PiΠ is symmetric with Πii=1\Pi_{ii}=1Πii​=1. What is observed is Yt∈{0,1}n×nY^t\in\{0,1\}^{n\times n}Yt∈{0,1}n×n, symmetric with zero diagonal, whose entries YijtY^t_{ij}Yijt​, i<ji<ji<j, are independent Bernoulli variables with success probability (Π⊙Θt)ij(\Pi\odot\Theta^t)_{ij}(Π⊙Θt)ij​, independent over ttt; ⊙\odot⊙ is the entrywise product.

The column-wise norm ∥M∥1,∞=max⁡j∑i∣Mij∣\|M\|_{1,\infty}=\max_j\sum_i|M_{ij}|∥M∥1,∞​=maxj​∑i​∣Mij​∣ measures the largest expected observed degree. The null class is

Sn(ωn)={(Θ,Π): Θ∈Cn0, Π∈Cn, ∥Π⊙Θ∥1,∞≤ωn}.\mathcal S_n(\omega_n)=\{(\Theta,\Pi):\ \Theta\in\mathcal C^0_n,\ \Pi\in\mathcal C_n,\ \|\Pi\odot\Theta\|_{1,\infty}\le\omega_n\}.Sn​(ωn​)={(Θ,Π): Θ∈Cn0​, Π∈Cn​, ∥Π⊙Θ∥1,∞​≤ωn​}.

A change at time τ∈{1,…,T−1}\tau\in\{1,\dots,T-1\}τ∈{1,…,T−1} replaces Θb=Θ0\Theta^b=\Theta^0Θb=Θ0 by Θa=Θ0+ΔΘτ\Theta^a=\Theta^0+\Delta\Theta^\tauΘa=Θ0+ΔΘτ after time τ\tauτ. With q(x)=x(1−x)q(x)=\sqrt{x(1-x)}q(x)=x(1−x)​ and the spectral norm ∥⋅∥2→2\|\cdot\|_{2\to2}∥⋅∥2→2​, the change-point energy is q(τ/T)∥Π⊙ΔΘτ∥2→2q(\tau/T)\|\Pi\odot\Delta\Theta^\tau\|_{2\to2}q(τ/T)∥Π⊙ΔΘτ∥2→2​, and the alternative class Wn,Tτ(ωn,r)\mathcal W^\tau_{n,T}(\omega_n,r)Wn,Tτ​(ωn​,r) collects the pairs in Sn(ωn)\mathcal S_n(\omega_n)Sn​(ωn​) whose energy is at least rrr.

A test ψ\psiψ maps the data to {0,1}\{0,1\}{0,1}. Its type I error α(ψ)\alpha(\psi)α(ψ) is the supremum over the null class of the probability of rejecting, and its type II error β(ψ,R)\beta(\psi,R)β(ψ,R) is the supremum over Wn,Tτ(ωn,R)\mathcal W^\tau_{n,T}(\omega_n,R)Wn,Tτ​(ωn​,R) of the probability of accepting.

The Matrix CUSUM is

ZT(t)=t(T−t)T(1t∑s=1tYs−1T−t∑s=t+1TYs),1≤t≤T−1,Z_T(t)=\sqrt{\frac{t(T-t)}{T}}\Big(\frac1t\sum_{s=1}^tY^s-\frac1{T-t}\sum_{s=t+1}^TY^s\Big),\qquad 1\le t\le T-1,ZT​(t)=Tt(T−t)​​(t1​s=1∑t​Ys−T−t1​s=t+1∑T​Ys),1≤t≤T−1,

and the test at the known time τ\tauτ is

ψn,Tτ(Y)=1{∥ZT(τ)∥2→2>Hα,n},Hα,n=22(1+ϵ)ωn+Cϵlog⁡(2n/α),\psi^\tau_{n,T}(Y)=\mathbf 1\big\{\|Z_T(\tau)\|_{2\to2}>H_{\alpha,n}\big\},\qquad H_{\alpha,n}=2\sqrt2(1+\epsilon)\sqrt{\omega_n}+C_\epsilon\log(2n/\alpha),ψn,Tτ​(Y)=1{∥ZT​(τ)∥2→2​>Hα,n​},Hα,n​=22​(1+ϵ)ωn​​+Cϵ​log(2n/α),

with ϵ∈(0,1/2]\epsilon\in(0,1/2]ϵ∈(0,1/2] and CϵC_\epsilonCϵ​ a constant depending only on ϵ\epsilonϵ.

Formalization targets

Goal: Theorem 1

For every ϵ∈(0,1/2]\epsilon\in(0,1/2]ϵ∈(0,1/2] there are constants Cϵ>0C_\epsilon>0Cϵ​>0 and CCC, depending only on ϵ\epsilonϵ, such that for all n≥1n\ge1n≥1, 1≤τ≤T−11\le\tau\le T-11≤τ≤T−1, ωn≥0\omega_n\ge0ωn​≥0 and α,β∈(0,1)\alpha,\beta\in(0,1)α,β∈(0,1): if

Rn,τ≥42(1+ϵ)(ωnT)1/2+CT1/2log⁡(nα∧β),R_{n,\tau}\ge4\sqrt2(1+\epsilon)\Big(\frac{\omega_n}{T}\Big)^{1/2}+\frac{C}{T^{1/2}}\log\Big(\frac{n}{\alpha\wedge\beta}\Big),Rn,τ​≥42​(1+ϵ)(Tωn​​)1/2+T1/2C​log(α∧βn​),

then α(ψn,Tτ)≤α\alpha(\psi^\tau_{n,T})\le\alphaα(ψn,Tτ​)≤α and β(ψn,Tτ,Rn,τ)≤β\beta(\psi^\tau_{n,T},R_{n,\tau})\le\betaβ(ψn,Tτ​,Rn,τ​)≤β. The constants are existential and are not pinned to particular values; the statement asserts the shape of the boundary.

Milestones

  1. Display (7): ZT(t)=−μTτ(t) Π⊙ΔΘτ+ξ(t)Z_T(t)=-\mu^\tau_T(t)\,\Pi\odot\Delta\Theta^\tau+\xi(t)ZT​(t)=−μTτ​(t)Π⊙ΔΘτ+ξ(t), with ξ(t)\xi(t)ξ(t) the CUSUM of the centred observations, and max⁡tμTτ(t)=μTτ(τ)=T q(τ/T)\max_t\mu^\tau_T(t)=\mu^\tau_T(\tau)=\sqrt T\,q(\tau/T)maxt​μTτ​(t)=μTτ​(τ)=T​q(τ/T).
  2. Proposition 11 (Bandeira and van Handel): for a symmetric m×mm\times mm×m matrix WWW with independent centred entries bounded by σ∗\sigma_*σ∗​,
P{∥W∥2→2≥22(1+ϵ)σ+x}≤m e−x2/(cϵσ∗2).\mathbb P\{\|W\|_{2\to2}\ge2\sqrt2(1+\epsilon)\sigma+x\}\le m\,e^{-x^2/(c_\epsilon\sigma_*^2)}.P{∥W∥2→2​≥22​(1+ϵ)σ+x}≤me−x2/(cϵ​σ∗2​).
  1. Lemma 12: with probability larger than 1−δ1-\delta1−δ,
∥ξ(t)∥2→2≤22(1+ϵ)t(T−t)T[1t2∑s≤t∥Bs∥1,∞+1(T−t)2∑s>t∥Bs∥1,∞]1/2+Cϵlog⁡2nδ.\|\xi(t)\|_{2\to2}\le2\sqrt2(1+\epsilon)\sqrt{\tfrac{t(T-t)}{T}}\Big[\tfrac1{t^2}\sum_{s\le t}\|B^s\|_{1,\infty}+\tfrac1{(T-t)^2}\sum_{s>t}\|B^s\|_{1,\infty}\Big]^{1/2}+C_\epsilon\log\tfrac{2n}{\delta}.∥ξ(t)∥2→2​≤22​(1+ϵ)Tt(T−t)​​[t21​s≤t∑​∥Bs∥1,∞​+(T−t)21​s>t∑​∥Bs∥1,∞​]1/2+Cϵ​logδ2n​.
  1. Lemma 3: the test has type I error at most α\alphaα.
  2. Lemma 4: under Rn,τ≥42(1+ϵ)(ωn/T)1/2+CϵT−1/2(log⁡(2n/α)+log⁡(2n/β))R_{n,\tau}\ge4\sqrt2(1+\epsilon)(\omega_n/T)^{1/2}+C_\epsilon T^{-1/2}(\log(2n/\alpha)+\log(2n/\beta))Rn,τ​≥42​(1+ϵ)(ωn​/T)1/2+Cϵ​T−1/2(log(2n/α)+log(2n/β)) the type II error is at most β\betaβ.

Significance

Theorem 1 is the upper half of the minimax detection boundary for a change at a known time. Together with Theorem 2 of the same paper (a lower bound of order (ωn/T)1/2(\omega_n/T)^{1/2}(ωn​/T)1/2) it shows that, up to the logarithmic term, the CUSUM test in spectral norm is rate-optimal, and that missing links enter only through the observed degree bound ωn=max⁡∥Π⊙Θ∥1,∞\omega_n=\max\|\Pi\odot\Theta\|_{1,\infty}ωn​=max∥Π⊙Θ∥1,∞​. The same noise bound (Lemma 12) drives the unknown-time test of Theorem 3.

The result is proved in the paper; no machine-checked version exists. Formalizing it produces a checked finite-sample statement with explicit leading constant 42(1+ϵ)4\sqrt2(1+\epsilon)42​(1+ϵ), a reusable formal Bernoulli network model with missing links, and, through Proposition 11, a formal statement of the Bandeira–van Handel tail bound, which is used well beyond change-point problems. The printed proof of Lemma 12 applies Proposition 11 after conditioning on the event {∥ξ(t)∥∞≤σ∗}\{\|\xi(t)\|_\infty\le\sigma_*\}{∥ξ(t)∥∞​≤σ∗​}, which destroys centring and independence; a complete proof needs a truncation argument that the paper does not give.

Difficulty

Under the null the CUSUM is pure noise, so both errors reduce to a high-probability bound on ∥ξ(t)∥2→2\|\xi(t)\|_{2\to2}∥ξ(t)∥2→2​ whose leading term is exactly 22(1+ϵ)ωn2\sqrt2(1+\epsilon)\sqrt{\omega_n}22​(1+ϵ)ωn​​ after rescaling. Matrix Bernstein inequalities give a bound with an extra log⁡n\sqrt{\log n}logn​ factor on the leading term, which is too weak for the stated threshold; the sharp constant requires the Bandeira–van Handel inequality, whose proof goes through moment comparisons for random matrices with non-identically distributed entries. The entries of ξ(t)\xi(t)ξ(t) are themselves sums over time with coefficients up to order T\sqrt TT​ in aggregate, so the boundedness hypothesis of Proposition 11 does not hold directly and must be recovered with probability bounds. Finally, the level and the power must hold for the same threshold constant CϵC_\epsilonCϵ​, uniformly in nnn, TTT, τ\tauτ and the parameters.

Formalization scope

An observation is a function from the TTT snapshots and the pairs i<ji<ji<j to Booleans; time is 0-based in Lean (snapshot sss is the paper's s+1s+1s+1). The latent adjacency and sampling matrices are integrated out: only YYY is modelled, by its exact product-Bernoulli law, and probabilities are finite sums over the finite observation space, so every test is measurable. Tests are Boolean-valued (true rejects). The sampling class carries the paper's standing assumptions Πii=1\Pi_{ii}=1Πii​=1 and Πij>0\Pi_{ij}>0Πij​>0. Errors are real suprema over sets contained in [0,1][0,1][0,1]; an empty alternative class has type II error 000. The spectral norm is the published HighDimProb.RandomMatrices.matrixOpNorm. Proposition 11 alone uses measure theory, with independence of the entries on and above the diagonal and an added (implicit) m≥1m\ge1m≥1.

Disclosed readings: (24) prints κn\kappa_nκn​, which is read as ωn\omega_nωn​ as in the proof; Lemma 12's matrices are the symmetric, zero-diagonal centred observations of the model; Lemmas 3 and 4 take "CϵC_\epsilonCϵ​ is a constant of Lemma 12" (with Cϵ>0C_\epsilon>0Cϵ​>0) as a hypothesis, stated as a predicate. The goal does not assume that predicate: it asserts the existence of CϵC_\epsilonCϵ​ and CCC, both chosen before nnn, TTT, τ\tauτ, ωn\omega_nωn​, α\alphaα, β\betaβ and RRR, so neither constant can be tuned to the instance, and tests range over all functions of the data. Choosing huge constants does not trivialize the goal, since for large TTT the energy condition is met by nonempty alternatives that the test must detect.

The development needs: the product-Bernoulli law of the network, the Matrix CUSUM algebra, the Bandeira–van Handel inequality, and a truncation argument for Lemma 12. The Setting and Proposition 11 are reusable for the unknown-time test and for spectral methods on random graphs. Proofs of any milestone, and alternative routes to Lemma 12, are welcome.

Selected references

  • F. Enikeeva and O. Klopp, Change-point detection in dynamic networks with missing links, Operations Research, 2025; arXiv:2106.14470v2. https://arxiv.org/abs/2106.14470
  • A. S. Bandeira and R. van Handel, Sharp nonasymptotic bounds on the norm of random matrices with independent entries, Annals of Probability 44(4), 2016. https://doi.org/10.1214/15-AOP1025
  • Yu. I. Ingster and I. A. Suslina, Nonparametric Goodness-of-Fit Testing under Gaussian Models, Springer, 2003. https://doi.org/10.1007/978-0-387-21580-8
9 thms1 active userReviewed
Numerical AnalysisProbability·Captain: tc

Gaussian Random Matrices II: Inverse Moments of the PseudoinverseTextbook

Motivation

The expected error of the randomized SVD with a k×(k+p)k\times(k+p)k×(k+p) Gaussian test matrix is (1+kp−1)1/2\bigl(1+\tfrac{k}{p-1}\bigr)^{1/2}(1+p−1k​)1/2 times the optimal error (Halko–Martinsson–Tropp 2011, Theorem 10.5). The factor kp−1\tfrac{k}{p-1}p−1k​ is E∥G†∥F2\mathbb E\|G^{\dagger}\|_F^2E∥G†∥F2​ for a k×(k+p)k\times(k+p)k×(k+p) standard Gaussian matrix GGG: the quality of every Gaussian sketching method is governed by inverse moments of a Gaussian matrix — moments of its pseudoinverse, equivalently of the inverse of the Wishart matrix GGTGG^{\mathsf T}GGT. The expected spectral error uses E∥G†∥\mathbb E\|G^{\dagger}\|E∥G†∥ instead (Tropp–Webber 2023, Lemmas B.2–B.3), and deviation bounds use tail estimates for both norms (HMT Proposition 10.4). None of these inverse moments is available in Mathlib. This mission proves them.

Setting

A standard Gaussian matrix G∈Rr×kG\in\mathbb R^{r\times k}G∈Rr×k has independent N(0,1)\mathcal N(0,1)N(0,1) entries; its law is γr,k\gamma_{r,k}γr,k​. Throughout, GGG is wide or square, r≤kr\le kr≤k, so that GGT∈Rr×rGG^{\mathsf T}\in\mathbb R^{r\times r}GGT∈Rr×r is almost surely invertible; GGTGG^{\mathsf T}GGT is a Wishart matrix with kkk degrees of freedom and (GGT)−1(GG^{\mathsf T})^{-1}(GGT)−1 is inverse-Wishart.

The pseudoinverse of a full-row-rank matrix is G†=GT(GGT)−1G^{\dagger}=G^{\mathsf T}(GG^{\mathsf T})^{-1}G†=GT(GGT)−1. Its norms are determined by the inverse Wishart matrix:

∥G†∥F2=tr⁡(GGT)−1,∥G†∥2=∥(GGT)−1∥=σmin⁡(G)−2,\|G^{\dagger}\|_F^2=\operatorname{tr}(GG^{\mathsf T})^{-1},\qquad \|G^{\dagger}\|^2=\|(GG^{\mathsf T})^{-1}\|=\sigma_{\min}(G)^{-2},∥G†∥F2​=tr(GGT)−1,∥G†∥2=∥(GGT)−1∥=σmin​(G)−2,

where ∥⋅∥F\|\cdot\|_F∥⋅∥F​ is the Frobenius norm, ∥⋅∥\|\cdot\|∥⋅∥ the spectral norm (largest singular value) and σmin⁡(G)\sigma_{\min}(G)σmin​(G) the smallest of the rrr singular values of GGG. The letter eee denotes Euler's number.

Formalization targets

Goal — Tropp–Webber inverse spectral moment (Lemma B.3)

For integer 1≤p≤181\le p\le181≤p≤18 and k≥r+2pk\ge r+2pk≥r+2p,

(E ∥(GGT)−1∥p)1/p≤e2(k+r)2(k−r)2.\Bigl(\mathbb E\,\bigl\|(GG^{\mathsf T})^{-1}\bigr\|^p\Bigr)^{1/p}\le\frac{e^2(k+r)}{2(k-r)^2}.(E​(GGT)−1​p)1/p≤2(k−r)2e2(k+r)​.

The case p=1p=1p=1 is E∥G†∥2≤e2(k+r)/(2(k−r)2)\mathbb E\|G^{\dagger}\|^2\le e^2(k+r)/(2(k-r)^2)E∥G†∥2≤e2(k+r)/(2(k−r)2), the spectral inverse moment at the heart of expected spectral-norm error bounds. It is the goal because it is the one inverse moment that is not an exact formula: its proof passes through Edelman's bound on the density of λmin⁡(GGT)\lambda_{\min}(GG^{\mathsf T})λmin​(GGT) and an explicit integration, and it implies the expectation bound of HMT Proposition 10.2 by Jensen's inequality.

Milestones

  • Inverse-Wishart mean. E(GGT)−1=1k−r−1Ir\mathbb E(GG^{\mathsf T})^{-1}=\frac{1}{k-r-1}I_rE(GGT)−1=k−r−11​Ir​ for r≤k−2r\le k-2r≤k−2 (Tropp–Webber Lemma B.2).
  • Frobenius inverse moment. E∥G†∥F2=rk−r−1\mathbb E\|G^{\dagger}\|_F^2=\frac{r}{k-r-1}E∥G†∥F2​=k−r−1r​ for k−r≥2k-r\ge2k−r≥2 (HMT Proposition 10.2 (10.3) and A.5).
  • Second-order inverse-Wishart moments. E∥G†∥F4=r2(k−r)−2r(r−1)(k−r)(k−r−1)(k−r−3)\mathbb E\|G^{\dagger}\|_F^4=\frac{r^2(k-r)-2r(r-1)}{(k-r)(k-r-1)(k-r-3)}E∥G†∥F4​=(k−r)(k−r−1)(k−r−3)r2(k−r)−2r(r−1)​ and E∥(GGT)−1∥F2=r(k−1)(k−r)(k−r−1)(k−r−3)\mathbb E\|(GG^{\mathsf T})^{-1}\|_F^2=\frac{r(k-1)}{(k-r)(k-r-1)(k-r-3)}E∥(GGT)−1∥F2​=(k−r)(k−r−1)(k−r−3)r(k−1)​ for r≤k−4r\le k-4r≤k−4 (Tropp–Webber Lemma B.2).
  • Chen–Dongarra tail. P{∥G†∥>t}≤12π(k−r+1)(ekk−r+1)k−r+1t−(k−r+1)\mathbb P\{\|G^{\dagger}\|>t\}\le\frac{1}{\sqrt{2\pi(k-r+1)}}\bigl(\frac{e\sqrt k}{k-r+1}\bigr)^{k-r+1}t^{-(k-r+1)}P{∥G†∥>t}≤2π(k−r+1)​1​(k−r+1ek​​)k−r+1t−(k−r+1) for k≥r≥2k\ge r\ge2k≥r≥2, t>0t>0t>0 (HMT Proposition A.3).
  • Expected spectral norm of the pseudoinverse. E∥G†∥≤ekk−r\mathbb E\|G^{\dagger}\|\le\frac{e\sqrt k}{k-r}E∥G†∥≤k−rek​​ for r≥2r\ge2r≥2, k≥r+1k\ge r+1k≥r+1 (HMT Proposition 10.2 (10.4) and A.4).
  • Frobenius tail. P{∥G†∥F2>12rk−rt}≤4t−(k−r)/2\mathbb P\{\|G^{\dagger}\|_F^2>\frac{12r}{k-r}t\}\le4t^{-(k-r)/2}P{∥G†∥F2​>k−r12r​t}≤4t−(k−r)/2 for k−r≥4k-r\ge4k−r≥4, t≥1t\ge1t≥1 (HMT Theorem A.6).

Significance

The results. Combined with the second-moment identity and block independence of Mission I, the Frobenius inverse moment gives the expected Frobenius error of the randomized SVD and of generalized Nyström; the spectral inverse moment gives the expected spectral error and the core-noise bounds of truncated sketching methods; the two tail bounds give the large-deviation statements of HMT §10.3. The second-order inverse-Wishart moments quantify the variance of ∥G†∥F2\|G^{\dagger}\|_F^2∥G†∥F2​, which Tropp–Webber use for concentration of the randomized SVD error.

Formalizing them. The inverse-Wishart mean and the second-order moments are classical multivariate-statistics formulas (Muirhead; von Rosen) with no Mathlib counterpart. The Chen–Dongarra tail requires the exact distribution of σmin⁡\sigma_{\min}σmin​, or at least Edelman's density bound; the Frobenius tail is HMT's own argument through the bidiagonal (Householder) model of a Gaussian matrix and chi-square moment estimates. Every statement here is a proved theorem in the literature; none has a machine-checked proof.

Difficulty

There is no Wishart distribution in Mathlib. The direct approach — compute the density of GGTGG^{\mathsf T}GGT and integrate — needs the Wishart density, a change of variables on the cone of positive-definite matrices, and the matrix-variate gamma function. The classical route to the mean avoids this: by rotational invariance (GGT)−1(GG^{\mathsf T})^{-1}(GGT)−1 has the same law as Q(GGT)−1QTQ(GG^{\mathsf T})^{-1}Q^{\mathsf T}Q(GGT)−1QT for every orthogonal QQQ, so its mean is a multiple of the identity, and the trace is ∑i1/χk−r+12\sum_i 1/\chi^2_{k-r+1}∑i​1/χk−r+12​-type quantities whose means are elementary; making "the diagonal entries of (GGT)−1(GG^{\mathsf T})^{-1}(GGT)−1 are reciprocals of χk−r+12\chi^2_{k-r+1}χk−r+12​ variables" rigorous requires the Gram–Schmidt (QR) decomposition of a Gaussian matrix and the independence of its factors. The spectral inverse moment needs a lower-tail bound for λmin⁡(GGT)\lambda_{\min}(GG^{\mathsf T})λmin​(GGT) of the exact order t(k−r+1)/2t^{(k-r+1)/2}t(k−r+1)/2; a union bound over rows loses a factor rrr and does not give the stated constant. The naive attempt to bound E∥G†∥2\mathbb E\|G^{\dagger}\|^2E∥G†∥2 by E∥G†∥F2\mathbb E\|G^{\dagger}\|_F^2E∥G†∥F2​ loses a factor rrr as well.

Formalization scope

GGG is sampled from the product measure γr,k\gamma_{r,k}γr,k​ on arrays; (⋅)−1(\cdot)^{-1}(⋅)−1 is Mathlib's total matrix inverse, equal to 000 on the null set where GGTGG^{\mathsf T}GGT is singular, and G†G^{\dagger}G† is defined as GT(GGT)−1G^{\mathsf T}(GG^{\mathsf T})^{-1}GT(GGT)−1 (pinvR). Every inequality is stated together with integrability of its integrand, so the Lean convention that a non-integrable function integrates to 000 cannot make a bound vacuous; identities with nonzero right-hand sides force integrability on their own but are also stated with it. The inverse-Wishart mean is stated entrywise. Tail bounds are inequalities between a measure in [0,∞][0,\infty][0,∞] and ofReal⁡\operatorname{ofReal}ofReal of the real bound. Real powers with non-integer exponents are Mathlib's rpow; all bases are positive under the hypotheses. The spectral norm is Mathlib's ℓ2\ell_2ℓ2​ operator norm. The sizes follow Tropp–Webber (G∈Rr×kG\in\mathbb R^{r\times k}G∈Rr×k); HMT's k×(k+p)k\times(k+p)k×(k+p) and m×nm\times nm×n conventions are translated in each item's source field.

Welcome contributions: a Wishart/inverse-Wishart library (QR decomposition of a Gaussian matrix, Bartlett decomposition, chi-square moments E Ξ−q=Γ(k/2−q)/(2qΓ(k/2))\mathbb E\,\Xi^{-q}=\Gamma(k/2-q)/(2^q\Gamma(k/2))EΞ−q=Γ(k/2−q)/(2qΓ(k/2))), and the distribution of σmin⁡\sigma_{\min}σmin​ of a Gaussian matrix (Edelman).

Selected references

  • N. Halko, P.-G. Martinsson, J. A. Tropp, Finding structure with randomness: probabilistic algorithms for constructing approximate matrix decompositions, SIAM Review 53(2), 217–288, 2011. https://arxiv.org/abs/0909.4061
  • J. A. Tropp, R. J. Webber, Randomized algorithms for low-rank matrix approximation: design, analysis, and applications, 2023. https://arxiv.org/abs/2306.12418
  • R. Vershynin, Introduction to the non-asymptotic analysis of random matrices, in Compressed Sensing: Theory and Applications, Cambridge University Press, 2012. https://arxiv.org/abs/1011.3027
  • L. Isserlis, On a formula for the product-moment coefficient of any order of a normal frequency distribution in any number of variables, Biometrika 12, 134–139, 1918. https://doi.org/10.1093/biomet/12.1-2.134
  • S. Dasgupta, A. Gupta, An elementary proof of a theorem of Johnson and Lindenstrauss, Random Structures & Algorithms 22, 60–65, 2003. https://doi.org/10.1002/rsa.10073
  • M. Rudelson, R. Vershynin, The Littlewood–Offord problem and invertibility of random matrices, Advances in Mathematics 218, 600–633, 2008. https://arxiv.org/abs/math/0703503
  • Y. Chen, J. Dongarra, Condition numbers of Gaussian random matrices, SIAM J. Matrix Anal. Appl. 27(3), 603–620, 2005. https://doi.org/10.1137/040616413
  • A. Edelman, Eigenvalues and condition numbers of random matrices, SIAM J. Matrix Anal. Appl. 9(4), 543–560, 1988. https://doi.org/10.1137/0609045
  • Y. Gordon, Some inequalities for Gaussian processes and applications, Israel J. Math. 50, 265–289, 1985. https://doi.org/10.1007/BF02759761
  • K. R. Davidson, S. J. Szarek, Local operator theory, random matrices and Banach spaces, Handbook of the Geometry of Banach Spaces, Vol. 1, 317–366, 2001. https://doi.org/10.1016/S1874-5849(01)80010-3
  • M. Ledoux, The Concentration of Measure Phenomenon, AMS Mathematical Surveys and Monographs 89, 2001. https://doi.org/10.1090/surv/089

Shared definitions: the items of this mission import Definitions.Def_GaussianMatrix_basic, a draft of Mission I; submit that proposal first so the import resolves at compile time.

Series: I. Rotation Invariance and Moment Identities · II. Inverse Moments of the Pseudoinverse · III. Extreme Singular Values and Concentration. All three missions share the definition bundle GaussianMatrix_basic, published with Mission I, and the namespace GaussianMatrix.

13 thms1 active userReviewed
Graph TheoryProbability·Captain: mikedeng1

Spectral Statistics of Erdős–Rényi Graphs I: Local Semicircle Law: Local Semicircle Law for the Sparse Noncentered Matrix A = H + f|e⟩⟨e| Down to Spectral Scale η ≈ 1/NResearch Paper

Motivation

The adjacency matrix of an Erdős–Rényi random graph contains a large deterministic mean as well as random fluctuations. The mean affects the largest eigenvalue, while the centered fluctuations determine much of the remaining spectrum. A local spectral law must describe both pieces at a resolution fine enough to distinguish eigenvalues within a narrow energy window. Erdős, Knowles, Yau and Yin established such estimates for a broader class of sparse symmetric matrices and their noncentered rank-one deformations in Spectral statistics of Erdős–Rényi graphs I. This mission formalizes the paper's Theorem 2.9, with the centered-matrix law and eleven intermediate results of the paper as milestones.

The paper treats the graph matrix through a model that also allows other sparse distributions. Its parameters qNq_NqN​ and fNf_NfN​ separate sparsity from the size of the deterministic mean. That separation matters: the normalized resolvent trace can obey a local semicircle law even when the deformation produces a distinguished top eigenvalue. The formal target therefore concerns the deformed matrix itself, rather than replacing it with the centered matrix.

Setting

For each size NNN, let HN=(hij)H_N=(h_{ij})HN​=(hij​) be a real symmetric random matrix. Entries indexed by the upper triangle are independent, centered, and have variance 1/N1/N1/N. Their higher moments obey

E∣hij∣p≤CpNqNp−2,3≤p≤(log⁡N)A0log⁡log⁡N.\mathbf E|h_{ij}|^p\le\frac{C^p}{Nq_N^{p-2}},\qquad 3\le p\le(\log N)^{A_0\log\log N}.E∣hij​∣p≤NqNp−2​Cp​,3≤p≤(logN)A0​loglogN.

The sparsity parameter qNq_NqN​ lies between (log⁡N)3ξN(\log N)^{3\xi_N}(logN)3ξN​ and CNC\sqrt NCN​, and the logarithmic parameter satisfies 1+a0≤ξN≤A0log⁡log⁡N1+a_0\le\xi_N\le A_0\log\log N1+a0​≤ξN​≤A0​loglogN, with a0>0a_0>0a0​>0 and A0≥10A_0\ge10A0​≥10. Define eN=N−1/2(1,…,1)e_N=N^{-1/2}(1,\ldots,1)eN​=N−1/2(1,…,1) and the noncentered matrix AN=HN+fN∣eN⟩⟨eN∣A_N=H_N+f_N|e_N\rangle\langle e_N|AN​=HN​+fN​∣eN​⟩⟨eN​∣, where 0≤fN≤NC0\le f_N\le N^C0≤fN​≤NC. The projection ∣eN⟩⟨eN∣|e_N\rangle\langle e_N|∣eN​⟩⟨eN​∣ has every entry equal to 1/N1/N1/N. These are Definitions 2.1 and 2.2 of the source paper, pp. 5–6.

For a complex number z=E+iηz=E+i\etaz=E+iη with η>0\eta>0η>0, the resolvents are G(z)=(HN−zI)−1G(z)=(H_N-zI)^{-1}G(z)=(HN​−zI)−1 and G~(z)=(AN−zI)−1\widetilde G(z)=(A_N-zI)^{-1}G(z)=(AN​−zI)−1. Their normalized traces are m(z)=N−1Tr⁡G(z)m(z)=N^{-1}\operatorname{Tr}G(z)m(z)=N−1TrG(z) and m~(z)=N−1Tr⁡G~(z)\widetilde m(z)=N^{-1}\operatorname{Tr}\widetilde G(z)m(z)=N−1TrG(z). The comparison object is the semicircle density ρsc(x)=(2π)−1[4−x2]+\rho_{\mathrm{sc}}(x)=(2\pi)^{-1}\sqrt{[4-x^2]_+}ρsc​(x)=(2π)−1[4−x2]+​​ and its Stieltjes transform msc(z)=∫Rρsc(x)/(x−z) dxm_{\mathrm{sc}}(z)=\int_{\mathbb R}\rho_{\mathrm{sc}}(x)/(x-z)\,dxmsc​(z)=∫R​ρsc​(x)/(x−z)dx. Put κE=∣∣E∣−2∣\kappa_E=\bigl||E|-2\bigr|κE​=​∣E∣−2​ and D={E+iη:∣E∣≤Σ, 0<η≤3}D=\{E+i\eta:|E|\le\Sigma,\ 0<\eta\le3\}D={E+iη:∣E∣≤Σ, 0<η≤3} for a fixed Σ≥3\Sigma\ge3Σ≥3. These definitions appear in Section 2, pp. 7–9.

An NNN-dependent event has (ξ,ν)(\xi,\nu)(ξ,ν)-high probability when its failure probability is at most exp⁡[−ν(log⁡N)ξN]\exp[-\nu(\log N)^{\xi_N}]exp[−ν(logN)ξN​] for all sufficiently large NNN. The spectral estimates below refer to single events on which the claimed bound holds at every z∈Dz\in Dz∈D simultaneously.

Formalization targets

Main goal: the local law for A

Theorem 2.9 assumes ξN∼(A0/2)log⁡log⁡N\xi_N\sim(A_0/2)\log\log NξN​∼(A0​/2)loglogN and qN≥(log⁡N)C1ξNq_N\ge(\log N)^{C_1\xi_N}qN​≥(logN)C1​ξN​. Its first conclusion is that, with (ξ,ν)(\xi,\nu)(ξ,ν)-high probability, every z=E+iη∈Dz=E+i\eta\in Dz=E+iη∈D satisfies

∣m~(z)−msc(z)∣≤(log⁡N)C2ξN(min⁡{1qN2κE+η,1qN}+1Nη).|\widetilde m(z)-m_{\mathrm{sc}}(z)|\le(\log N)^{C_2\xi_N}\left(\min\left\{\frac1{q_N^2\sqrt{\kappa_E+\eta}},\frac1{q_N}\right\}+\frac1{N\eta}\right).∣m(z)−msc​(z)∣≤(logN)C2​ξN​(min{qN2​κE​+η​1​,qN​1​}+Nη1​).

Under the additional bound fN≤C0Nf_N\le C_0\sqrt NfN​≤C0​N​, its second conclusion controls every entry at every z∈Dz\in Dz∈D:

∣G~ij(z)−δijmsc(z)∣≤(log⁡N)C2ξN(1qN+Im⁡msc(z)Nη+1Nη).|\widetilde G_{ij}(z)-\delta_{ij}m_{\mathrm{sc}}(z)|\le(\log N)^{C_2\xi_N}\left(\frac1{q_N}+\sqrt{\frac{\operatorname{Im}m_{\mathrm{sc}}(z)}{N\eta}}+\frac1{N\eta}\right).∣Gij​(z)−δij​msc​(z)∣≤(logN)C2​ξN​(qN​1​+NηImmsc​(z)​​+Nη1​).

The constants C1,C2C_1,C_2C1​,C2​ are universal and positive. The probability exponent ν>0\nu>0ν>0 may depend on the fixed parameters named in the theorem. Both conclusions, including the extra condition on fNf_NfN​ in the second, are retained from Theorem 2.9, pp. 9–10.

Milestones

The milestones follow the paper's own sequence of numbered results.

  1. Properties of mscm_{\mathrm{sc}}msc​ (Lemma 3.2): ∣msc∣∼1|m_{\mathrm{sc}}|\sim1∣msc​∣∼1, ∣1−msc2∣∼κE+η|1-m_{\mathrm{sc}}^2|\sim\sqrt{\kappa_E+\eta}∣1−msc2​∣∼κE​+η​, and the size of Im⁡msc\operatorname{Im}m_{\mathrm{sc}}Immsc​ inside and outside the spectrum.
  2. Resolvent identities for minors (Lemma 3.4) and the self-consistent equation Gii=1/(−z−msc−([v]−Υi))G_{ii}=1/(-z-m_{\mathrm{sc}}-([v]-\Upsilon_i))Gii​=1/(−z−msc​−([v]−Υi​)) (Lemma 3.10); both are deterministic.
  3. Large deviation bounds for linear and quadratic forms in independent variables with the sparse moment decay (Lemma 3.8 (ii)).
  4. The weak local semicircle law for HHH (Theorem 3.1) on DL={∣E∣≤Σ, (log⁡N)LN−1≤η≤3}D_L=\{|E|\le\Sigma,\ (\log N)^LN^{-1}\le\eta\le3\}DL​={∣E∣≤Σ, (logN)LN−1≤η≤3}, L≥8ξL\ge8\xiL≥8ξ.
  5. Fluctuation averaging (Lemma 4.1 (4.2)): the average [Z]=N−1∑iZi[Z]=N^{-1}\sum_iZ_i[Z]=N−1∑i​Zi​ of the fluctuation terms is much smaller than each ZiZ_iZi​.
  6. The a priori norm bound ∥H∥≤2+(log⁡N)ξq−1/2\|H\|\le2+(\log N)^\xi q^{-1/2}∥H∥≤2+(logN)ξq−1/2 (Lemma 4.3) and the strong local law for HHH (Theorem 2.8, the analogue of the goal for f=0f=0f=0).
  7. Interlacing of the eigenvalues of HHH and AAA (Lemma 6.1) and the near-orthogonality ∑α≠N∣⟨vα,e⟩∣2=O(f−2)\sum_{\alpha\ne N}|\langle v_\alpha,e\rangle|^2=O(f^{-2})∑α=N​∣⟨vα​,e⟩∣2=O(f−2) of eee to the non-top eigenvectors of AAA (Corollary 6.7).
  8. The trace comparison ∣Λ~−Λ∣≤π/(Nη)|\widetilde\Lambda-\Lambda|\le\pi/(N\eta)∣Λ−Λ∣≤π/(Nη) (Lemma 7.1), which yields the first conclusion of the goal from Theorem 2.8.
  9. Entrywise control of G~\widetilde GG on the event Ω~(η)\widetilde\Omega(\eta)Ω(η) that Λ~d+Λ~o≤(log⁡N)−ξ\widetilde\Lambda_d+\widetilde\Lambda_o\le(\log N)^{-\xi}Λd​+Λo​≤(logN)−ξ on the line Im⁡z=η\operatorname{Im}z=\etaImz=η: the off-diagonal bound Λ~o≤CΦ\widetilde\Lambda_o\le C\PhiΛo​≤CΦ (Proposition 7.6 (7.14)) and the diagonal bounds of Lemma 7.7, with Φ=(log⁡N)ξ/q+(log⁡N)2ξ(Im⁡m~/(Nη)+1/(Nη))\Phi=(\log N)^\xi/q+(\log N)^{2\xi}(\sqrt{\operatorname{Im}\widetilde m/(N\eta)}+1/(N\eta))Φ=(logN)ξ/q+(logN)2ξ(Imm/(Nη)​+1/(Nη)).

Significance

The trace estimate gives quantitative control over spectral mass at local scales, including near the edges E=±2E=\pm2E=±2. The entrywise estimate says more: each resolvent entry is close to the diagonal semicircle approximation with an error that records both sparsity and finite-size effects. The paper's later results derive density-of-states and eigenvector statements from these local controls. Those consequences are outside this mission's goal.

The intended formal development supplies reusable definitions of sparse symmetric ensembles, high-probability events, semicircle transforms, and complex resolvents, followed by exact statements of the paper's estimates. Mathlib contains no local semicircle law, for Wigner or for sparse matrices, and no Stieltjes transform of the semicircle distribution; the local law, the large deviation bounds and the interlacing lemma are each reusable beyond this paper.

Difficulty

The deterministic rank-one comparison controls the normalized trace but does not by itself control each entry of G~\widetilde GG. The entrywise estimate must account for the deformation and for fluctuations caused by sparse entries. Near the spectral edges, the stability scale of the semicircle transform changes with κE+η\kappa_E+\etaκE​+η; a bound that is uniform in the bulk does not automatically retain the paper's edge behavior. The theorem also asks for one event covering a continuum of zzz values, so a collection of separate fixed-zzz probability bounds has the wrong quantifier order. These are substantive parts of Sections 3–7, beyond algebraic manipulation of resolvents.

Formalization scope

Lean represents all HNH_NHN​ on one probability space and takes their entries to be real, symmetric, measurable random variables, independent in the upper triangle. Conditions involving log⁡log⁡N\log\log NloglogN and the moments hold for all sufficiently large NNN; this avoids impossible small-NNN parameter bounds and matches the asymptotic theorem. The moment order ppp is real, as in the paper. Each finite expectation has an explicit integrability condition. A single positive constant CCC is used for the moment, sparsity, and deformation bounds: replacing several fixed constants by their maximum preserves all three inequalities.

Matrix indices use Fin N rather than the paper's 1,…,N1,\ldots,N1,…,N. The resolvent is a complex matrix formed by coercing the real matrix before subtracting zIzIzI. Every result that uses it restricts η>0\eta>0η>0 eventually or explicitly; its inverse at a singular input is never used to make a claim. The semicircle transform is defined by the paper's integral, and 4−x2\sqrt{4-x^2}4−x2​ uses Lean's nonnegative square root, implementing the positive part. The high-probability predicate evaluates the measure of arbitrary sets, so it can state the intersection over all zzz without a separate measurability assumption on that intersection. Positive qNq_NqN​ and positive square-root arguments follow eventually from the model and z∈Dz\in Dz∈D.

The deterministic Lemmas 3.2, 3.4, 3.10, 6.1 and 7.1 are stated for every real symmetric matrix and every zzz with η>0\eta>0η>0 (Lemma 3.2 on DDD); the paper's DLD_LDL​ is contained there. Minors keep the original index names, and Gkl(T)G^{(\mathbb T)}_{kl}Gkl(T)​ is only used for k,l∉Tk,l\notin\mathbb Tk,l∈/T. ZiZ_iZi​ is the explicit expression of (3.15). Ordered eigenvalues are the sorted roots of the characteristic polynomial. Statements the paper makes "for fixed zzz" (Lemmas 4.1, 7.7, Proposition 7.6) are uniform in zzz: one threshold N0N_0N0​ serves every zzz. The unnamed constants CCC, ν\nuν, KKK are chosen after the fixed parameters and before the random matrices; the universal C1,C2C_1,C_2C1​,C2​ come first.

Trivializing encodings are ruled out: every resolvent is taken at η>0\eta>0η>0, so the junk inverse of a singular matrix never enters; the model is satisfiable (independent Rademacher signs divided by N\sqrt NN​ with qN=Nq_N=\sqrt NqN​=N​ and ξN=(A0/2)log⁡log⁡N\xi_N=(A_0/2)\log\log NξN​=(A0​/2)loglogN satisfy it for large NNN); each event of the goal is one intersection over all z∈Dz\in Dz∈D, not a family of pointwise bounds; the constants appear in the paper's order; and the goal is about A=H+f∣e⟩⟨e∣A=H+f|e\rangle\langle e|A=H+f∣e⟩⟨e∣ with fff allowed to be large, so it does not reduce to Theorem 2.8.

Part (iii) of Lemma 3.8 is not a milestone: the printed (3.22) omits the diagonal variance term (N−2∑i∣Bii∣2)1/2(N^{-2}\sum_i|B_{ii}|^2)^{1/2}(N−2∑i​∣Bii​∣2)1/2, without which it fails for Rademacher variables with q≍Nq\asymp\sqrt Nq≍N​. Contributions of proofs of any milestone, and of the missing groundwork (Stieltjes transforms of measures, Schur complements of resolvents, moment bounds for sums of independent variables), are welcome.

Selected references

  • L. Erdős, A. Knowles, H.-T. Yau and J. Yin, Spectral statistics of Erdős–Rényi graphs I: Local semicircle law, Annals of Probability 41(3B), 2013, pp. 2279–2375. arXiv:1103.1919v5; DOI:10.1214/11-AOP734.
16 thms1 active userReviewed
Information TheoryProbabilityStatistics·Captain: mikedeng1

Universality in Polytope Phase Transitions and Message Passing Algorithms 2: State Evolution, Empirical Averages of Polynomial AMP Iterates Converge to Gaussian ExpectationsResearch Paper

Motivation

Approximate message passing (AMP) is an iterative method for large systems with random matrices. At each step, every coordinate receives a weighted combination of nonlinear messages from all other coordinates, together with a correction for dependence created by earlier steps. For symmetric random matrices, the correction makes a simple description of the high-dimensional iterates possible: a finite collection of covariance matrices predicts their limiting distributions. Bayati, Lelarge and Montanari prove this state evolution statement for polynomial AMP on a broad class of independent sub-Gaussian matrix entries, rather than only Gaussian entries (paper, §§1.2–1.3). It gives a precise distributional account of an algorithm whose coordinates are coupled at every iteration.

The paper has three distinct headline results. Its Theorem 3 compares AMP moments under two matrix laws with equal entry variances, and its Theorem 2 concerns projected cross-polytopes. This mission targets Theorem 4, which identifies the limit of empirical averages of AMP iterates with a Gaussian expectation. The companion missions address the other results; the statements here use their own copy of the paper's AMP model because draft definitions cannot yet be imported across proposals (paper, pp. 5, 8–9).

Setting

For each size NNN, let A(N)A(N)A(N) be a random symmetric N×NN\times NN×N matrix with zero diagonal. Its entries above the diagonal are independent, centered, and sub-Gaussian at scale C/NC/NC/N. Each coordinate iii carries a polynomial map fi(⋅;t):Rq→Rqf^i(\cdot;t):\mathbb R^q\to\mathbb R^qfi(⋅;t):Rq→Rq at iteration ttt and an initial vector xi0x_i^0xi0​. Their coefficients have degree at most ddd and a uniform bound CCC. The AMP orbit is

xit+1=∑jAijfj(xjt;t)−∑jAij2Jfj(xjt;t)fi(xit−1;t−1).x_i^{t+1}=\sum_j A_{ij}f^j(x_j^t;t) -\sum_j A_{ij}^{2}Jf^j(x_j^t;t)f^i(x_i^{t-1};t-1).xit+1​=j∑​Aij​fj(xjt​;t)−j∑​Aij2​Jfj(xjt​;t)fi(xit−1​;t−1).

The second sum is the Onsager memory term; it is absent at t=0t=0t=0. Here JfjJf^jJfj is the Jacobian, so its product with the preceding qqq-vector is another qqq-vector. The initial vectors obey an exponential bound on their squared Euclidean norms. These assumptions form the paper's (C,d)(C,d)(C,d)-regularity condition (Definitions 2–4, pp. 6–7).

A converging sequence has a fixed finite set of classes a∈[k]a\in[k]a∈[k]. Coordinate iii belongs to CaNC_a^NCaN​ for one class aaa, whose proportion approaches ca∈(0,1)c_a\in(0,1)ca​∈(0,1). A symmetric nonnegative matrix WWW specifies entry variances: if i∈CaNi\in C_a^Ni∈CaN​ and j∈CbNj\in C_b^Nj∈CbN​, then EAij2=Wab/N\mathbb E A_{ij}^2=W_{ab}/NEAij2​=Wab​/N. Independent labels Y(i)Y(i)Y(i) have class-dependent laws PaP_aPa​, each a finite mixture of Gaussian laws that may be degenerate. The polynomial maps have the common form fi(x;t)=g(x,Y(i),a,t)f^i(x;t)=g(x,Y(i),a,t)fi(x;t)=g(x,Y(i),a,t) for i∈CaNi\in C_a^Ni∈CaN​ (Definition 5, pp. 8–9).

The empirical second moments of g(xi0,Y(i),a,0)g(x_i^0,Y(i),a,0)g(xi0​,Y(i),a,0) converge in probability to a prescribed positive semidefinite matrix Σ^a0\widehat\Sigma_a^0Σa0​. For t≥1t\ge1t≥1, state evolution defines

Σat=∑bcbWabΣ^bt−1,Σ^at=E[g(Zat,Ya,a,t)g(Zat,Ya,a,t)T],\Sigma_a^t=\sum_b c_bW_{ab}\widehat\Sigma_b^{t-1},\qquad \widehat\Sigma_a^t=\mathbb E\big[g(Z_a^t,Y_a,a,t)g(Z_a^t,Y_a,a,t)^{\mathsf T}\big],Σat​=b∑​cb​Wab​Σbt−1​,Σat​=E[g(Zat​,Ya​,a,t)g(Zat​,Ya​,a,t)T],

where Zat∼N(0,Σat)Z_a^t\sim\mathcal N(0,\Sigma_a^t)Zat​∼N(0,Σat​) is independent of Ya∼PaY_a\sim P_aYa​∼Pa​. The index t−1t-1t−1 in the first formula and ttt in the second are essential (equations (1.9)–(1.11), p. 9).

Formalization targets

Coordinate moments and concentration

For a nonnegative multi-index mmm and a coordinate sequence eventually in class aaa, Proposition 4 identifies the Gaussian limit of each moment. Proposition 5 says the variance of the class-average monomial tends to zero:

E[(xi(N)t)m]⟶E[(Zat)m],Var⁡ ⁣(1∣CaN∣∑i∈CaN(xit)m)⟶0.\mathbb E[(x_{i(N)}^t)^m]\longrightarrow\mathbb E[(Z_a^t)^m],\qquad \operatorname{Var}\!\left(\frac1{|C_a^N|}\sum_{i\in C_a^N}(x_i^t)^m\right)\longrightarrow0.E[(xi(N)t​)m]⟶E[(Zat​)m],Var​∣CaN​∣1​i∈CaN​∑​(xit​)m​⟶0.

The diagonal two-time identity (4.4) is another milestone: Σat,t\Sigma_a^{t,t}Σat,t​ has four blocks, each equal to Σat\Sigma_a^tΣat​. These are the paper's stated intermediate targets (pp. 15, 30, 32).

Main goal: Theorem 4

For t≥1t\ge1t≥1, class aaa, and every locally Lipschitz function ψ\psiψ with ∣ψ(x,y)∣≤K(1+∥x∥22+∥y∥22)K|\psi(x,y)|\le K(1+\|x\|_2^2+\|y\|_2^2)^K∣ψ(x,y)∣≤K(1+∥x∥22​+∥y∥22​)K for some KKK, prove convergence in probability:

1∣CaN∣∑j∈CaNψ(xjt,Y(j))⟶E[ψ(Zat,Ya)].\frac1{|C_a^N|}\sum_{j\in C_a^N}\psi(x_j^t,Y(j)) \longrightarrow \mathbb E[\psi(Z_a^t,Y_a)].∣CaN​∣1​j∈CaN​∑​ψ(xjt​,Y(j))⟶E[ψ(Zat​,Ya​)].

The target covers polynomial-growth test functions, including functions beyond monomials. The expectation on the right is under the product law of the Gaussian state and the independent class label (Theorem 4, p. 9).

Significance

The theorem assigns a computable asymptotic distribution to each class of AMP coordinates at every fixed positive iteration time. It can be used to evaluate empirical observables without tracking the full coupled NNN-dimensional random trajectory. The class weights and variance profile permit heterogeneous coordinates, while the sub-Gaussian assumption covers more matrix laws than a Gaussian-only statement (paper, Introduction and Theorem 4).

The paper proves this result. The mission's Lean statements are compilation-checked targets, with proofs still to be formalized. A completed development would establish the measure-theoretic meaning of the covariance recursion and its Gaussian expectations, as well as the moment and concentration claims needed for the empirical limit. The polynomial representation, random-matrix regularity predicate, and Gaussian transport are reusable for other AMP results from the same paper.

Difficulty

The matrix A(N)A(N)A(N) is reused at every AMP iteration, so a new coordinate is correlated with earlier coordinates and with the matrix entries that produced them. A direct independent-summand argument for its Gaussian limit is unavailable. The memory term is tuned to this dependence, and any formal proof must account for its exact Jacobian and squared-entry form. Passing from individual moments to empirical averages also requires control of correlations between different coordinates. The target allows locally Lipschitz functions with polynomial growth, so convergence for a fixed monomial alone does not finish the job (paper, §4.7).

Formalization scope

Vectors in Rq\mathbb R^qRq are functions Fin q → ℝ; squared Euclidean norms are explicit sums of coordinate squares. Polynomials use bounded real coefficient arrays as in (4.10), with an explicit Jacobian. Fin N uses zero-based indices. The orbit stores the current and preceding iterates and omits the memory term at t=0t=0t=0. A single probability space carries all sizes; matrix entries, labels, coefficients, and initial vectors have explicit measurability and independence conditions.

The paper's displayed sub-Gaussian formula conflicts with its stated C/NC/NC/N scale, so the model uses the scale required by its moment estimates and imposes the moment-generating bound for all real arguments. Its initial exponential bound is read almost surely at every size, which ensures the expectations used by the paper are well-defined. Label-dependent polynomial coefficients are measurable. The full label vector is independent of the matrix and initial vectors; this makes explicit the independence needed for Theorem 4's Gaussian-label product law. Independence of the induced polynomial coefficients alone would not imply it when ggg ignores part of a label. The initial covariance limit is entrywise convergence in probability; finite-dimensional equivalence makes this the same matrix convergence. Class averages divide by the class cardinality, even though that expression has Lean's default value at an empty class for a small NNN. Positive limiting class fractions make those finite exceptions irrelevant.

Gaussian laws live on Mathlib's Euclidean space and are transported to coordinate vectors. Theorems explicitly assert positive semidefiniteness or integrability where a non-PSD covariance, non-integrable expectation, or non-square-integrable variance could otherwise give a default value. The source's Y(i)Y(i)Y(i) in (1.12) is read as Y(j)Y(j)Y(j), its summation index, and its final covariance as Σat\Sigma_a^tΣat​. The Gaussian covariance is computed by the recursion above; it is not defined from the proposed limit. Contributions establishing moment bounds, covariance positivity, Gaussian integrability, the three milestones, or the full Theorem 4 are within scope.

Selected references

  • M. Bayati, M. Lelarge and A. Montanari, Universality in polytope phase transitions and message passing algorithms, Annals of Applied Probability 25(2), 2015, 753–822. arXiv:1207.7321v2; DOI:10.1214/14-AAP1010.
12 thms1 active userReviewed
Convex OptimizationDiscrete GeometryInformation Theory+1·Captain: mikedeng1

Universality in Polytope Phase Transitions and Message Passing Algorithms 3: Projected Cross-Polytopes Have Weak Neighborliness ρ∗(δ) for Sub-Gaussian Matrices with a Gaussian ComponentResearch Paper

Why this phase transition matters

Sparse recovery asks when a vector with few nonzero coordinates can be reconstructed from fewer linear measurements than unknowns. A related geometric question asks how many faces of a high-dimensional cross-polytope survive a random linear projection. The two questions meet at the same threshold: uniqueness of a minimum-one-norm solution corresponds to a face of the projected cross-polytope. For Gaussian measurement matrices this threshold was known before the work of Bayati, Lelarge and Montanari, from Donoho's face-counting analysis (Donoho 2006); the same curve was later identified as the transition of approximate message passing (Donoho, Maleki and Montanari 2009). Their 2015 paper establishes the same weak-neighborliness curve for a broader class of independent sub-Gaussian entries with a nonzero Gaussian component. The result addresses the universality question posed for these projections: does the asymptotic transition depend on the full entry distribution or only on broad features of the matrix law?

The mathematical theorem is established in that paper. This mission records its statement in Lean and leaves the machine-checked proof open. The relevant statement is Theorem 2 on page 5 of the pinned arXiv version 2, rather than a claim about every random projection without a Gaussian component.

Polytopes, faces, and random matrices

The cross-polytope CnC_nCn​ is the unit ball for the coordinate one-norm in Rn\mathbb R^nRn:

Cn={x∈Rn:∑i=1n∣xi∣≤1}.C_n=\left\{x\in\mathbb R^n:\sum_{i=1}^n|x_i|\leq1\right\}.Cn​={x∈Rn:i=1∑n​∣xi​∣≤1}.

For an m×nm\times nm×n matrix AAA, the projected polytope ACnAC_nACn​ consists of all AxAxAx with x∈Cnx\in C_nx∈Cn​. Write F(Q;ℓ)F(Q;\ell)F(Q;ℓ) for the number of nonempty faces of QQQ whose affine dimension is ⌊ℓ⌋\lfloor\ell\rfloor⌊ℓ⌋. The weak neighborliness level ρ∈(0,1)\rho\in(0,1)ρ∈(0,1) of a random sequence Qn⊆Rm(n)Q_n\subseteq\mathbb R^{m(n)}Qn​⊆Rm(n) means that, for every ξ>0\xi>0ξ>0, the ratio F(Qn;m(n)ρ(1−ξ))/F(Cn;m(n)ρ(1−ξ))F(Q_n;m(n)\rho(1-\xi))/F(C_n;m(n)\rho(1-\xi))F(Qn​;m(n)ρ(1−ξ))/F(Cn​;m(n)ρ(1−ξ)) converges in probability to one, while the analogous ratio with 1+ξ1+\xi1+ξ converges in probability to zero. Both limits belong to the definition; the first alone would record only survival below a candidate threshold.

The matrices have m(n)=⌊nδ⌋m(n)=\lfloor n\delta\rfloorm(n)=⌊nδ⌋ rows for a fixed sampling ratio δ∈(0,1)\delta\in(0,1)δ∈(0,1). Within each matrix, the entries are independent, centered, unit-variance, and sub-Gaussian with one scale factor independent of nnn. They also admit a decomposition A(n)=A~(n)+ν0G(n)A(n)=\widetilde A(n)+\nu_0G(n)A(n)=A(n)+ν0​G(n), where ν0>0\nu_0>0ν0​>0 and the entries of G(n)G(n)G(n) are independent standard normal variables, jointly independent of A~(n)\widetilde A(n)A(n). The theorem imposes no independence between matrices with different values of nnn Bayati–Lelarge–Montanari, Theorem 2.

Formalization targets

Let ϕ\phiϕ and Φ\PhiΦ be the density and distribution function of a standard normal random variable. The paper defines its phase boundary through a positive parameter α\alphaα:

fδ(α)=2ϕ(α)α+2(ϕ(α)−αΦ(−α)),fρ(α)=1−αΦ(−α)ϕ(α).f_\delta(\alpha)=\frac{2\phi(\alpha)}{\alpha+2\bigl(\phi(\alpha)-\alpha\Phi(-\alpha)\bigr)},\qquad f_\rho(\alpha)=1-\frac{\alpha\Phi(-\alpha)}{\phi(\alpha)}.fδ​(α)=α+2(ϕ(α)−αΦ(−α))2ϕ(α)​,fρ​(α)=1−ϕ(α)αΦ(−α)​.

Footnote 3 states that fδf_\deltafδ​ decreases from one to zero on the nonnegative half-line, so each δ∈(0,1)\delta\in(0,1)δ∈(0,1) has exactly one positive parameter. The goal, Theorem 2, says that whenever fδ(α)=δf_\delta(\alpha)=\deltafδ​(α)=δ, the sequence A(n)CnA(n)C_nA(n)Cn​ has weak neighborliness fρ(α)f_\rho(\alpha)fρ​(α) in probability. The Lean theorem spells out this parameter relation; it does not apply an inverse function at an argument outside a proved range.

The milestone list covers the two scalar results identifying the boundary, a deterministic condition for exact recovery, and the compressed-sensing transition. With ZZZ standard normal and u+=max⁡(u,0)u_+=\max(u,0)u+​=max(u,0), the scalar function is

Gε(α)=ε(1+α2)+2(1−ε)E[(Z−α)+2].G_\varepsilon(\alpha)=\varepsilon(1+\alpha^2)+2(1-\varepsilon)\mathbb E[(Z-\alpha)_+^2].Gε​(α)=ε(1+α2)+2(1−ε)E[(Z−α)+2​].

Lemma 8 gives its unique positive minimizer and its minimum value. Lemma 9 relates that minimum to both sides of the boundary. The scalar state evolution σt+12=F(σt2,ασt)\sigma_{t+1}^2=\mathsf F(\sigma_t^2,\alpha\sigma_t)σt+12​=F(σt2​,ασt​), with F(σ2,θ)=δ−1E{[η(X+σZ;θ)−X]2}\mathsf F(\sigma^2,\theta)=\delta^{-1}\mathbb E\{[\eta(X+\sigma Z;\theta)-X]^2\}F(σ2,θ)=δ−1E{[η(X+σZ;θ)−X]2} and η(u;θ)=sign⁡(u)(∣u∣−θ)+\eta(u;\theta)=\operatorname{sign}(u)(|u|-\theta)_+η(u;θ)=sign(u)(∣u∣−θ)+​ soft thresholding, has slope Gε(α)/δG_\varepsilon(\alpha)/\deltaGε​(α)/δ at the origin and is concave (Lemma 7). Lemma 10 shows that a two-time correlation map Fα,ε\mathcal F_{\alpha,\varepsilon}Fα,ε​ satisfies Fα,ε(Q)>Q\mathcal F_{\alpha,\varepsilon}(Q)>QFα,ε​(Q)>Q on [0,1)[0,1)[0,1). Theorem 10, cited from Bürgisser and Cucker, bounds the probability that a Gaussian-perturbed rectangular matrix has a small least singular value:

P{σN(B+νG)≤νz}≤(a1z)M−N+1.\mathbb P\{\sigma_N(B+\nu G)\le\nu z\}\le(a_1z)^{M-N+1}.P{σN​(B+νG)≤νz}≤(a1​z)M−N+1.

Lemma 5 gives a recovery condition based on an approximate dual certificate and singular-value bounds. Theorem 8 states that minimum-one-norm recovery succeeds with probability tending to one below the boundary and fails with probability tending to one above it Bayati–Lelarge–Montanari, pp. 39–41, 60–61.

What a formal proof would establish

The goal would certify that the same face-count transition applies to every entry law in the stated class, including laws that are not identically distributed across the matrix. The conclusion is geometric: it counts faces of an actual projected one-norm ball. The recovery milestone provides a second way to state the threshold for sparse signals. Together they make the normalization and the two sides of the transition explicit, so future variants can compare their assumptions and conclusions with a fixed formal statement.

No machine-checked proof of Theorem 2 or of the selected milestones is known. The declarations are open Lean statements over explicit definitions. A complete development would formalize the known argument in the paper, including the probabilistic estimates and the bridge from recovery probabilities to face counts. Sharper results that remove the Gaussian component would be separate theorems with their own hypotheses.

Where the difficulty lies

The count of surviving faces depends on many supports and sign patterns simultaneously. Matching means and variances of matrix entries does not make their finite-dimensional face counts equal. Likewise, controlling recovery for one fixed signal does not immediately control the fraction of all faces. Near the boundary, exact recovery also requires uniform singular-value information for many column submatrices. These are the points where elementary concentration for a single entry or a single support is insufficient. The source paper treats the geometric statement and the recovery transition under a Gaussian-component condition; a proof that silently assumes full Gaussianity would miss its universality claim.

Formalization scope

Vectors are functions on Fin n, and every one-norm is an explicit sum of absolute values. The squared Euclidean norm is a sum of coordinate squares; the default norm on Fin n → ℝ is not used for it. Face counts reuse the published Grunbaum2003.faceCount definition, with dimension ⌊ℓ⌋\lfloor\ell\rfloor⌊ℓ⌋ for nonnegative ℓ\ellℓ; negative dimensions have zero nonempty faces. The two limits in weak neighborliness use convergence in measure, which expresses convergence in probability here. The printed lower ratio has a zero denominator for ξ>1\xi>1ξ>1, so that limit is stated for 0<ξ≤10<\xi\leq10<ξ≤1. Ratios at small nnn may involve zero denominators, but the asymptotic assertion concerns arbitrarily large nnn.

Theorem 2 uses variance one and an N(0,1)N(0,1)N(0,1) Gaussian component. Theorem 8 instead uses variance 1/m(n)1/m(n)1/m(n) and an N(0,1/m(n))N(0,1/m(n))N(0,1/m(n)) component, exactly as printed. Sub-Gaussianity uses Mathlib's moment-generating-function predicate for all real parameters; this is the operative two-sided reading of the paper's stated scale condition. The scalar Gaussian expectation in GεG_\varepsilonGε​ is accompanied by an explicit integrability conclusion in Lemma 8, excluding Lean's zero value for a nonintegrable integral. The restricted least singular value is the infimum of output norms on unit column vectors. This gives zero when a wide submatrix has a kernel and is the bound needed by Lemma 5. The state-evolution map is written as a function of σ2\sigma^2σ2, and its derivative at 000 is a right derivative. In Lemma 10 the law of X∞X_\inftyX∞​ is the three-atom mixture on {0,+∞,−∞}\{0,+\infty,-\infty\}{0,+∞,−∞}, with the split of the mass ε\varepsilonε between the two infinite atoms left free. The page's clause Fα,ε′(1)<1\mathcal F'_{\alpha,\varepsilon}(1)<1Fα,ε′​(1)<1 is stated for α>α∗(ε)\alpha>\alpha_*(\varepsilon)α>α∗​(ε), since the derivative equals 111 at α=α∗\alpha=\alpha_*α=α∗​. Theorem 10 quantifies ν>0\nu>0ν>0 and z>0z>0z>0, which the page leaves implicit.

The random-matrix predicates require measurability, independence within each nnn, the stated marginal laws, and independence of G(n)G(n)G(n) from A~(n)\widetilde A(n)A(n). They leave the matrix law otherwise arbitrary. The weak-neighborliness predicate contains both face-ratio limits and 0<ρ<10<\rho<10<ρ<1; neither the goal nor a milestone defines the threshold by assuming its conclusion. A full proof needs reusable facts about Gaussian integrals, independence of finite arrays, random face counts, restricted singular values, and the relation between projected faces and unique one-norm recovery. Contributions establishing those facts or closing any of the listed theorem statements are within scope.

Selected references

  • Mohsen Bayati, Marc Lelarge and Andrea Montanari, Universality in polytope phase transitions and message passing algorithms, Annals of Applied Probability 25(2), 2015. arXiv:1207.7321v2
  • David L. Donoho, High-dimensional centrally symmetric polytopes with neighborliness proportional to dimension, Discrete & Computational Geometry 35, 617–652, 2006. MR2225676
  • David L. Donoho, Arian Maleki and Andrea Montanari, Message-passing algorithms for compressed sensing, Proceedings of the National Academy of Sciences 106, 18914–18919, 2009. doi:10.1073/pnas.0909892106
  • Peter Bürgisser and Felipe Cucker, Smoothed analysis of Moore–Penrose inversion, SIAM Journal on Matrix Analysis and Applications 31, 2769–2783, 2010. MR2740632
16 thms1 active userReviewed
Linear algebraProbability·Captain: mikedeng1

User-Friendly Tail Bounds for Sums of Random Matrices III: The Matrix Chernoff Inequality for Sums of Independent Positive-Semidefinite Random MatricesResearch Paper

Motivation

The classical Chernoff bound controls the probability that a sum of independent, nonnegative, uniformly bounded random variables deviates from its mean, with exponentially small tails governed by the Kullback–Leibler divergence between two Bernoulli laws. Many problems in numerical linear algebra, graph sparsification, compressed sensing and randomized algorithms instead require control of a sum of independent random matrices: the smallest singular value of a random matrix with independent columns, the spectrum of a sampled Laplacian, or the conditioning of a random submatrix. For these, what matters is not a scalar sum but the extreme eigenvalues of a random positive-semidefinite matrix.

Ahlswede and Winter (2002) introduced a matrix version of the Laplace transform method and proved a matrix Chernoff bound for identically distributed summands. Tropp's paper (arXiv:1004.4389, Found. Comput. Math. 2012) replaced the Golden–Thompson step of their argument with Lieb's concavity theorem, obtaining a master tail bound for independent sums, and derived from it matrix Chernoff, Bernstein and Azuma inequalities that require no identical distribution and lose only a dimensional factor. This mission formalizes the matrix Chernoff inequalities of §5 of that paper.

Timeline:

  • 2002, Ahlswede–Winter: matrix Laplace transform method; matrix Chernoff bound for i.i.d. summands via Golden–Thompson.
  • 2010, Oliveira: a variant of the Laplace transform method used in Proposition 3.1 of the paper.
  • 2010–2012, Tropp: master tail bound via Lieb's theorem (Theorem 3.6), and Theorem 5.1 / Corollary 5.2 for independent, non-identical psd summands.

Setting

All matrices are d×dd\times dd×d complex matrices with d≥1d\ge1d≥1. For a self-adjoint (Hermitian) matrix AAA, λmax⁡(A)\lambda_{\max}(A)λmax​(A) and λmin⁡(A)\lambda_{\min}(A)λmin​(A) are its algebraically largest and smallest eigenvalues. The semidefinite order A≼BA\preccurlyeq BA≼B means that B−AB-AB−A is positive semidefinite (psd). Functions of a self-adjoint matrix are defined spectrally: if A=QΛQ∗A = Q\Lambda Q^*A=QΛQ∗ then f(A)=Qf(Λ)Q∗f(A) = Qf(\Lambda)Q^*f(A)=Qf(Λ)Q∗; this gives the matrix exponential eAe^AeA and, on positive-definite matrices, the matrix logarithm log⁡A\log AlogA.

A random matrix is a measurable map X:Ω→Cd×dX:\Omega\to\mathbb C^{d\times d}X:Ω→Cd×d on a probability space (Ω,F,P)(\Omega,\mathcal F,\mathbb P)(Ω,F,P), and its expectation EX\mathbb E XEX is taken entrywise. The matrix moment generating function of XXX is θ↦E eθX\theta\mapsto\mathbb E\,e^{\theta X}θ↦EeθX.

The objects of the mission are independent random Hermitian matrices X1,…,XnX_1,\dots,X_nX1​,…,Xn​ that are almost surely psd contractions: Xk≽0X_k\succcurlyeq0Xk​≽0 and λmax⁡(Xk)≤1\lambda_{\max}(X_k)\le1λmax​(Xk​)≤1. Their average expectation has extreme eigenvalues

μˉmin⁡=λmin⁡(1n∑k=1nEXk),μˉmax⁡=λmax⁡(1n∑k=1nEXk),\bar\mu_{\min} = \lambda_{\min}\Big(\frac1n\sum_{k=1}^n\mathbb E X_k\Big),\qquad \bar\mu_{\max}=\lambda_{\max}\Big(\frac1n\sum_{k=1}^n\mathbb E X_k\Big),μˉ​min​=λmin​(n1​k=1∑n​EXk​),μˉ​max​=λmax​(n1​k=1∑n​EXk​),

and the binary information divergence is

D(a ∥ u)=a(log⁡a−log⁡u)+(1−a)(log⁡(1−a)−log⁡(1−u)),a,u∈[0,1].\mathrm D(a\,\|\,u) = a(\log a-\log u)+(1-a)(\log(1-a)-\log(1-u)),\qquad a,u\in[0,1].D(a∥u)=a(loga−logu)+(1−a)(log(1−a)−log(1−u)),a,u∈[0,1].

In Lean these are lambdaMax, lambdaMin, mexp, mlog, mean and binDiv in the namespace MatrixTail.Chernoff.

Formalization targets

Goal: Theorem 5.1 (Matrix Chernoff I)

P{λmin⁡(1n∑kXk)≤α}≤d e−n D(α∥μˉmin⁡)(0≤α≤μˉmin⁡),\mathbb P\Big\{\lambda_{\min}\Big(\tfrac1n\textstyle\sum_k X_k\Big)\le\alpha\Big\}\le d\,e^{-n\,\mathrm D(\alpha\|\bar\mu_{\min})}\quad(0\le\alpha\le\bar\mu_{\min}),P{λmin​(n1​∑k​Xk​)≤α}≤de−nD(α∥μˉ​min​)(0≤α≤μˉ​min​), P{λmax⁡(1n∑kXk)≥α}≤d e−n D(α∥μˉmax⁡)(μˉmax⁡≤α≤1).\mathbb P\Big\{\lambda_{\max}\Big(\tfrac1n\textstyle\sum_k X_k\Big)\ge\alpha\Big\}\le d\,e^{-n\,\mathrm D(\alpha\|\bar\mu_{\max})}\quad(\bar\mu_{\max}\le\alpha\le1).P{λmax​(n1​∑k​Xk​)≥α}≤de−nD(α∥μˉ​max​)(μˉ​max​≤α≤1).

Milestones

  1. Theorem 3.6 (master tail bound): for every θ>0\theta>0θ>0 at which the mgfs exist, P{λmax⁡(∑kXk)≥t}≤e−θttr⁡exp⁡(∑klog⁡E eθXk)\mathbb P\{\lambda_{\max}(\sum_kX_k)\ge t\}\le e^{-\theta t}\operatorname{tr}\exp(\sum_k\log\mathbb E\,e^{\theta X_k})P{λmax​(∑k​Xk​)≥t}≤e−θttrexp(∑k​logEeθXk​).
  2. Corollary 3.9: the same with the mgfs under one logarithm, d⋅exp⁡(−θt+nlog⁡λmax⁡(1n∑kE eθXk))d\cdot\exp(-\theta t+n\log\lambda_{\max}(\frac1n\sum_k\mathbb E\,e^{\theta X_k}))d⋅exp(−θt+nlogλmax​(n1​∑k​EeθXk​)).
  3. Lemma 5.8 (Chernoff mgf): E eθX≼I+(eθ−1)EX\mathbb E\,e^{\theta X}\preccurlyeq\mathbf I+(e^\theta-1)\mathbb E XEeθX≼I+(eθ−1)EX for a random psd contraction XXX.
  4. Display (5.1): P{λmax⁡(∑kXk)≥t}≤dexp⁡(−θt+nlog⁡(1+(eθ−1)μˉmax⁡))\mathbb P\{\lambda_{\max}(\sum_kX_k)\ge t\}\le d\exp(-\theta t+n\log(1+(e^\theta-1)\bar\mu_{\max}))P{λmax​(∑k​Xk​)≥t}≤dexp(−θt+nlog(1+(eθ−1)μˉ​max​)).
  5. Display (5.2): P{λmin⁡(∑kXk)≤t}≤dexp⁡(θt+nlog⁡(1−(1−e−θ)μˉmin⁡))\mathbb P\{\lambda_{\min}(\sum_kX_k)\le t\}\le d\exp(\theta t+n\log(1-(1-e^{-\theta})\bar\mu_{\min}))P{λmin​(∑k​Xk​)≤t}≤dexp(θt+nlog(1−(1−e−θ)μˉ​min​)).

Further statement

Corollary 5.2 (Matrix Chernoff II), the form usually quoted: with λmax⁡(Xk)≤R\lambda_{\max}(X_k)\le Rλmax​(Xk​)≤R, μmin⁡,μmax⁡\mu_{\min},\mu_{\max}μmin​,μmax​ the extreme eigenvalues of ∑kEXk\sum_k\mathbb E X_k∑k​EXk​,

P{λmin⁡(∑kXk)≤(1−δ)μmin⁡}≤d[e−δ(1−δ)1−δ]μmin⁡/R,P{λmax⁡(∑kXk)≥(1+δ)μmax⁡}≤d[eδ(1+δ)1+δ]μmax⁡/R.\mathbb P\{\lambda_{\min}(\textstyle\sum_kX_k)\le(1-\delta)\mu_{\min}\}\le d\Big[\tfrac{e^{-\delta}}{(1-\delta)^{1-\delta}}\Big]^{\mu_{\min}/R},\quad \mathbb P\{\lambda_{\max}(\textstyle\sum_kX_k)\ge(1+\delta)\mu_{\max}\}\le d\Big[\tfrac{e^{\delta}}{(1+\delta)^{1+\delta}}\Big]^{\mu_{\max}/R}.P{λmin​(∑k​Xk​)≤(1−δ)μmin​}≤d[(1−δ)1−δe−δ​]μmin​/R,P{λmax​(∑k​Xk​)≥(1+δ)μmax​}≤d[(1+δ)1+δeδ​]μmax​/R.

Significance

Theorem 5.1 matches the strongest scalar Chernoff bound for independent, non-identical Bernoulli trials, up to the factor ddd, which cannot be removed (coupon collector, Remark 5.6). Corollary 5.2 is the version used in applications: lower bounds on the smallest singular value of matrices with independent columns (Remark 5.4), spectral sparsification, column subset selection and random sampling of matrices. Remark 5.5 derives from it the expectation bound Eλmax⁡(∑kXk)≤Cmax⁡{μmax⁡,Rlog⁡d}\mathbb E\lambda_{\max}(\sum_kX_k)\le C\max\{\mu_{\max},R\log d\}Eλmax​(∑k​Xk​)≤Cmax{μmax​,Rlogd}.

The results are proved in the paper, from Lieb's concavity theorem. As far as is known, no machine-checked proof of a matrix Chernoff inequality exists in Lean or Mathlib. A formalization yields a reusable statement for the random-matrix and randomized-numerical-linear-algebra literature, and the milestones (the master bound, the single-logarithm corollary and the semidefinite mgf bound) are reusable beyond this mission.

Difficulty

The scalar Chernoff argument uses E eθ(X+Y)=E eθX E eθY\mathbb E\,e^{\theta(X+Y)}=\mathbb E\,e^{\theta X}\,\mathbb E\,e^{\theta Y}Eeθ(X+Y)=EeθXEeθY for independent X,YX,YX,Y. For matrices eA+B≠eAeBe^{A+B}\neq e^Ae^BeA+B=eAeB unless AAA and BBB commute, so the trace of the mgf of a sum does not factor. The Golden–Thompson inequality handles two summands but does not extend to three, which is why the Ahlswede–Winter bound needed identical distributions. The master bound (Theorem 3.6) requires Lieb's concavity theorem, which has no counterpart in Mathlib. Corollary 3.9 in addition needs operator concavity of the matrix logarithm, and Lemma 5.8 needs the transfer of a scalar inequality to the semidefinite order through the spectral calculus.

Formalization scope

Matrices are Matrix (Fin d) (Fin d) ℂ with [NeZero d]; the semidefinite order is Mathlib's MatrixOrder (A ≤ B ↔ (B − A).PosSemidef). exp and log of a matrix are the continuous functional calculus cfc. λmax⁡\lambda_{\max}λmax​, λmin⁡\lambda_{\min}λmin​ are sSup/sInf of the real spectrum. Expectation is entrywise. Random matrices are measurable with respect to the Borel σ-algebra on matrices, independence is iIndepFun, and the probability measure is a probability measure. The summands are Hermitian for every outcome; "psd" and "λmax⁡≤1\lambda_{\max}\le1λmax​≤1" hold almost surely. The sequence has n≥1n\ge1n≥1 terms wherever an average 1/n1/n1/n appears. An infimum over θ>0\theta>0θ>0 is stated as a bound for every admissible θ>0\theta>0θ>0; integrability of eθXke^{\theta X_k}eθXk​ is a hypothesis only in Theorem 3.6 and Corollary 3.9, where the summands are unbounded. In Lean log⁡0=0\log 0=0log0=0, so at the boundary values μˉ∈{0,1}\bar\mu\in\{0,1\}μˉ​∈{0,1} the divergence is finite where the paper's is +∞+\infty+∞; this only weakens the stated bound.

A formalization in which d=0d=0d=0 (empty spectrum, λmax⁡=0\lambda_{\max}=0λmax​=0) or n=0n=0n=0 (the average 1/0=01/0=01/0=0) were allowed, or in which the range of α\alphaα were dropped, would state a different, partly false theorem; these cases are excluded.

A complete development needs Lieb's theorem or another route to the master bound, operator concavity of the logarithm, the spectral mapping theorem and the transfer rule for the functional calculus on Hermitian matrices, monotonicity of the trace exponential, and the scalar optimization in θ\thetaθ. Contributions of any of these as stand-alone lemmas are welcome.

Selected references

  • J. A. Tropp, User-Friendly Tail Bounds for Sums of Random Matrices, arXiv:1004.4389v7 (2011); Found. Comput. Math. 12 (2012) 389–434. https://arxiv.org/abs/1004.4389, https://doi.org/10.1007/s10208-011-9099-z
  • R. Ahlswede, A. Winter, Strong converse for identification via quantum channels, IEEE Trans. Inform. Theory 48 (2002) 569–579. https://doi.org/10.1109/18.985947
  • E. H. Lieb, Convex trace functions and the Wigner–Yanase–Dyson conjecture, Adv. Math. 11 (1973) 267–288. https://doi.org/10.1016/0001-8708(73)90011-X
  • R. I. Oliveira, Sums of random Hermitian matrices and an inequality by Rudelson, Electron. Commun. Probab. 15 (2010) 203–212. https://arxiv.org/abs/1004.3821
8 thms1 active userReviewed
PreviousPage 1 of 2Next

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

How Prove2Me worksResearch paper
SKILL.mdTourFAQContactTerms
© 2026 Prove2Me