Random Matrices: Universality of ESDs and the Circular Law 2: The ESD of A_n/√n Converges to μ iff the Normalized Log-Determinants of A_n/√n − zI Converge to μ's Log-Potential for a.e. zResearch Paper
Motivation
The eigenvalues of a large non-Hermitian random matrix are hard to study directly. For Hermitian matrices, the empirical spectral distribution (ESD) is controlled by the resolvent and the Stieltjes transform, both stable under small perturbations. For non-Hermitian matrices no such tool exists: eigenvalues can move a long way under tiny perturbations, and the moment method fails because moments do not determine a measure on . The route that works, going back to Girko (1984) and used by Bai (1997), Götze–Tikhomirov (2007), Pan–Zhou (2007) and Tao–Vu (2008), passes through logarithmic determinants. The identity links the ESD to a scalar quantity. That scalar is computable from the singular values of , which are eigenvalues of a Hermitian matrix.
Tao and Vu, with an appendix by Krishnapur (Ann. Probab. 38 (2010) 2023–2065), turn this link into an exact criterion. Theorem 1.15 of that paper states that the ESD of a normalized i.i.d. random matrix converges to a measure if and only if the normalized log-determinants converge to the logarithmic potential of for almost every . The same holds for a regularized version built from the singular values. This mission formalizes Theorem 1.15 and the main steps of its proof (§8 and Appendix A of the published article).
Setting
Let be a complex random variable with and , and let be independent copies of on a probability space . For each , . Let be deterministic complex matrices with
and put .
For with eigenvalues , counted with algebraic multiplicity, the ESD is . Its singular values are . A sequence of random measures converges in probability to a deterministic if, for every continuous compactly supported , tends to in probability. It converges almost surely if, with probability one, for all such at once. The logarithmic potential of a measure is .
Hypothesis (1.4) states that, for almost every , the ESDs of the deterministic matrices converge to a limit.
In Lean everything lives in the namespace UnivESD.LogDet. The ESD is esd, the one-based singular value is sv, logPotential is the logarithmic potential, and ConvInProb/ConvAS/ESDConvInProb/ESDConvAS are the modes of convergence. IIDArray is the entry model, HSBound is (1.3), shiftA M xs z n ω is , and Cond14 is (1.4).
Formalization targets
Goal: Theorem 1.15
Let be a probability measure on with . The following are equivalent:
- in probability;
- for a.e. , in probability;
- for a.e. there are , , with
in probability.
Under (1.4) the same equivalence holds with almost sure convergence throughout.
Milestones, in the order the proof uses them
- (8.1): for a.e. , is -integrable.
- Lemma A.3 (Weyl's comparison for products): and .
- (8.3): for .
- (8.2): almost surely.
- p. 2057: almost surely, eventually, , and the same bound for .
Significance
Theorem 1.15 reduces convergence of a non-Hermitian ESD to a family of scalar limit statements. Each of these can be attacked through Hermitian tools, because the regularized log-determinant in (iii) is a smooth functional of the singular values. Corollary 1.16 of the paper derives from it a practical criterion: the ESD converges to once the singular value distributions of converge for a.e. to laws with . With the universality principle (Theorem 1.5, the companion mission) and Mehta's computation for complex Gaussian matrices, this yields the circular law for i.i.d. matrices with finite variance.
The theorem is proved in the source. To our knowledge neither it nor any of its milestones has a machine-checked proof. Mathlib has the ingredients for the objects (characteristic polynomials and their roots, LinearMap.singularValues, the strong law of large numbers) but not the results. A formal proof would give the platform its first verified bridge between eigenvalue and singular value asymptotics. Lemma A.3 alone, Weyl's multiplicative majorization, is a standard linear-algebra fact absent from Mathlib.
Difficulty
Two things make the obvious argument fail. First, is unbounded at . Vague convergence of controls only for continuous compactly supported , while has a singularity at and grows at infinity. Passing between (i) and (ii) therefore requires uniform control of the eigenvalues (and singular values) near after the shift: the contribution of the smallest ones must vanish. Second, eigenvalues are not stable under perturbation, so this control cannot be read off the eigenvalues. It has to come from the singular values, through a lower-tail bound on that is exponentially small in a power of , and through a deterministic inequality transferring bounds from singular values to eigenvalues. The smallest singular values ( below ) need a separate polynomial lower bound (the paper's Lemma 4.1, posed in the companion mission). The tail bound in its printed form is false at that end of the range.
Formalization scope
Conventions committed to in Lean:
- The ESD is times the sum of Dirac masses over the root multiset of the characteristic polynomial, so multiplicities are kept. Test functions are real-valued, continuous and compactly supported. Almost sure ESD convergence uses one null set for all test functions.
- The matrices are the top-left corners of one infinite i.i.d. array. In-probability statements do not depend on how the are coupled across , but almost-sure statements do, and the paper's proof applies the strong law to this array. The limit in (1.4) is required to be a probability measure, which is equivalent under (1.3).
- The second-moment condition on is
Integrable (‖w‖²) μ. The logarithmic potential is a Bochner integral, which is when not integrable; by (8.1) this happens only for a null set of , which "for a.e. " ignores. Real.log 0 = 0. In (ii), a singular matrix would contribute instead of ; for this model the determinant is almost surely nonzero eventually. Every milestone with or carries positivity of those quantities in its conclusion.- Singular values are one-based (
sv A iis Mathlib'ssingularValues (i-1)). Eigenvalue enumerations areFin n-indexed, and the paper's is index . - The paper's constants are existential and fixed before . In the bounds the constant is fixed before ; a -dependent constant would make the bounds empty.
Disclosed corrections to the printed text:
- (iii)'s matrix. Theorem 1.15 prints a mis-bracketed product, and (1.8) prints . The Lean uses with , the matrix of (8.2) and of the proof of Corollary 1.16.
- (8.3)'s range. It is printed for , which is false for small : for Gaussian entries and , has a non-degenerate limit law. It is posed on , the range the proof covers and the use needs.
- Lemma A.3, second inequality. It is posed for , since is undefined. The eigenvalues are ordered , not as printed: the printed order is a slip. With it, both inequalities are weaker than Weyl's and cannot support the use on p. 2057, which orders the eigenvalues decreasingly. The decreasing order implies the printed form.
- (8.2) and (8.1). (8.2) is stated for every deterministic with ; the proof uses nothing else. (8.1) is stated as -integrability plus local integrability of .
A trivializing formalization is ruled out by construction. The goal mentions only and . The proof's comparison ensemble is not a hypothesis. No statement takes a log-potential or a log-determinant as an input that could be fixed to make it hold.
The companion mission (Theorem 1.5, universality) poses Theorem 2.1 (the replacement principle), Lemma 1.7 (tightness) and Lemma 4.1 (least singular value), which the proof here also uses. They are not restated here. Once that mission is published they belong here as references. Contributions are welcome on the linear-algebra layer (Lemma A.3, multiplicative Weyl majorization), the Fubini argument of (8.1), and the singular-value tail bound (8.3). These are reusable well beyond this paper.
Selected references
- T. Tao, V. Vu (appendix by M. Krishnapur), Random matrices: Universality of ESDs and the circular law, Ann. Probab. 38(5) (2010) 2023–2065. https://doi.org/10.1214/10-AOP534 (source of this mission; published version).
- V. L. Girko, The circular law, Teor. Veroyatnost. i Primenen. 29 (1984) 669–679. https://doi.org/10.1137/1129095
- Z. D. Bai, Circular law, Ann. Probab. 25(1) (1997) 494–529. https://doi.org/10.1214/aop/1024404298
- F. Götze, A. Tikhomirov, The circular law for random matrices, Ann. Probab. 38(4) (2010) 1444–1491. https://doi.org/10.1214/09-AOP522
- T. Tao, V. Vu, Random matrices: the circular law, Commun. Contemp. Math. 10(2) (2008) 261–307. https://doi.org/10.1142/S0219199708002788
- H. Weyl, Inequalities between the two kinds of eigenvalues of a linear transformation, Proc. Natl. Acad. Sci. USA 35 (1949) 408–411. https://doi.org/10.1073/pnas.35.7.408