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Edelman's density bound for λmin⁡\lambda_{\min}λmin​ of a Wishart matrix, integrated: P{λmin⁡(GG⊤)≤t}≤∫0tcr,kλ(k−r−1)/2e−λ/2dλ\mathbb P\{\lambda_{\min}(GG^\top)\le t\}\le\int_0^t c_{r,k}\lambda^{(k-r-1)/2}e^{-\lambda/2}d\lambdaP{λmin​(GG⊤)≤t}≤∫0t​cr,k​λ(k−r−1)/2e−λ/2dλ

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GaussianMatrix.wishart_lambda_min_cdf_density_bound

by tc · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

density-boundgaussian-matrixprobabilityrandom-matricessmallest-eigenvaluewishart-matrix

Let 1≤r≤k1\le r\le k1≤r≤k be integers and let GGG be an r×kr\times kr×k random matrix with independent standard normal entries, so that W=GG⊤W=GG^\topW=GG⊤ is a real Wishart matrix Wr(k,I)W_r(k,I)Wr​(k,I). Write

λmin⁡(GG⊤)=σmin⁡(G⊤)2,σmin⁡(G⊤)=inf⁡x∈Rr, ∥x∥2=1∥G⊤x∥2,\lambda_{\min}(GG^\top)=\sigma_{\min}(G^\top)^2,\qquad \sigma_{\min}(G^\top)=\inf_{x\in\mathbb R^r,\ \|x\|_2=1}\|G^\top x\|_2 ,λmin​(GG⊤)=σmin​(G⊤)2,σmin​(G⊤)=x∈Rr, ∥x∥2​=1inf​∥G⊤x∥2​,

and put

cr,k=2(k−r−1)/2 Γ ⁣(k+12)Γ ⁣(r2) Γ(k−r+1).c_{r,k}=\frac{2^{(k-r-1)/2}\,\Gamma\!\big(\frac{k+1}{2}\big)}{\Gamma\!\big(\frac r2\big)\,\Gamma(k-r+1)}.cr,k​=Γ(2r​)Γ(k−r+1)2(k−r−1)/2Γ(2k+1​)​.

Then for every t>0t>0t>0,

P{λmin⁡(GG⊤)≤t}  ≤  ∫0tcr,k λ(k−r−1)/2e−λ/2 dλ.\mathbb P\big\{\lambda_{\min}(GG^\top)\le t\big\}\;\le\;\int_0^t c_{r,k}\,\lambda^{(k-r-1)/2}e^{-\lambda/2}\,d\lambda .P{λmin​(GG⊤)≤t}≤∫0t​cr,k​λ(k−r−1)/2e−λ/2dλ.

This is the integrated form of Edelman's pointwise density bound fλmin⁡(λ)≤cr,kλ(k−r−1)/2e−λ/2f_{\lambda_{\min}}(\lambda)\le c_{r,k}\lambda^{(k-r-1)/2}e^{-\lambda/2}fλmin​​(λ)≤cr,k​λ(k−r−1)/2e−λ/2 for λ>0\lambda>0λ>0 (Tropp–Webber eq. (B.5)). Edelman's derivation starts from the joint eigenvalue density of WWW, ∝∏iλi(k−r−1)/2e−λi/2∏i<j∣λi−λj∣\propto\prod_i\lambda_i^{(k-r-1)/2}e^{-\lambda_i/2}\prod_{i<j}|\lambda_i-\lambda_j|∝∏i​λi(k−r−1)/2​e−λi​/2∏i<j​∣λi​−λj​∣. It writes fλmin⁡(λ)=λ(k−r−1)/2e−λ/2 h(λ)f_{\lambda_{\min}}(\lambda)=\lambda^{(k-r-1)/2}e^{-\lambda/2}\,h(\lambda)fλmin​​(λ)=λ(k−r−1)/2e−λ/2h(λ), where hhh is nonincreasing, and bounds h(λ)≤h(0+)=cr,kh(\lambda)\le h(0^+)=c_{r,k}h(λ)≤h(0+)=cr,k​. The bound is therefore sharp as λ→0+\lambda\to0^+λ→0+, and for r=1r=1r=1 it is an equality: c1,kλk/2−1e−λ/2c_{1,k}\lambda^{k/2-1}e^{-\lambda/2}c1,k​λk/2−1e−λ/2 is exactly the χk2\chi^2_kχk2​ density. Combined with tw_gamma_ratio_bound and integral_power_exp_le, it gives the lower-tail bound wishart_lambda_min_tail (TW (B.7)). That bound in turn gives the tail and moment bounds for ∥G†∥\|G^\dagger\|∥G†∥ and ∥(GG⊤)−1∥\|(GG^\top)^{-1}\|∥(GG⊤)−1∥.

Formalization Note. The law of GGG is gaussianMatrix r k on Fin r → Fin k → ℝ, and λmin⁡(GG⊤)\lambda_{\min}(GG^\top)λmin​(GG⊤) is written sMin (Matrix.of G)ᵀ ^ 2, so no eigenvalues need to be defined. The right-hand side is a lower Lebesgue integral (lintegral) over (0,t](0,t](0,t] of ENNReal.ofReal of the density bound. The integrand is integrable, since (k−r−1)/2≥−12>−1(k-r-1)/2\ge-\tfrac12>-1(k−r−1)/2≥−21​>−1, and the lintegral form avoids Bochner-integral junk values. Γ\GammaΓ is Real.Gamma, and the powers are real powers, positive on (0,t](0,t](0,t]. The hypothesis r≥1r\ge1r≥1 is necessary: for r=0r=0r=0, Real.Gamma 0 = 0 makes c0,k=0c_{0,k}=0c0,k​=0, while the event is the whole space. Only the interval form is stated, because it is all that (B.7) needs; it is weaker than the pointwise density bound.

Preamble
import Definitions.Def_GaussianMatrix_basic

open MeasureTheory ProbabilityTheory
open scoped Matrix
Formal statement
namespace GaussianMatrix

theorem wishart_lambda_min_cdf_density_bound {r k : ℕ} (hr : 1 ≤ r) (hrk : r ≤ k) (t : ℝ)
    (ht : 0 < t) :
    (gaussianMatrix r k) {G | sMin (Matrix.of G)ᵀ ^ 2 ≤ t}
      ≤ ∫⁻ x in Set.Ioc 0 t, ENNReal.ofReal
          (2 ^ (((k : ℝ) - r - 1) / 2) * Real.Gamma (((k : ℝ) + 1) / 2)
              / (Real.Gamma ((r : ℝ) / 2) * Real.Gamma ((k : ℝ) - r + 1))
            * x ^ (((k : ℝ) - r - 1) / 2) * Real.exp (-x / 2)) := by sorry

end GaussianMatrix
Source
A. Edelman, Eigenvalues and condition numbers of random matrices, SIAM J. Matrix Anal. Appl. 9(4) (1988) 543–560, Prop. 5.1 (density bound for λ_min of a real Wishart matrix; the proposition number is the one cited by Tropp–Webber and was not checked against the original); restated in J. A. Tropp and R. J. Webber, Randomized algorithms for low-rank matrix approximation: design, analysis, and applications, arXiv:2306.12418, Appendix B, proof of Lemma B.3, eq. (B.5) (after Legendre duplication of Edelman's constant). The statement here is the integral of (B.5) over (0, t].

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