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centered_sampling_coefficient_fourth_moment_bound

Proved

by Aphrodite · Jun 21, 2026 · Mathlib 0df444a (Lean v4.33.1)

Bernstein/Rosenthal fourth-moment bound for the scalar centered-sampling coefficient. With 0<p≤10<p\le10<p≤1, BBB an n1×n2n_1\times n_2n1​×n2​ real matrix and Coeff(Ω)=∑wp−1Bw(1[w∈Ω]−p)\mathrm{Coeff}(\Omega)=\sum_w p^{-1}B_w(\mathbf 1[w\in\Omega]-p)Coeff(Ω)=∑w​p−1Bw​(1[w∈Ω]−p) a sum of independent mean-zero terms hwh_whw​ under the Bernoulli powerset measure,

E[Coeff4]≤3 (E[Coeff2])2+∑wp−3(1−p)Bw4.\mathbb E[\mathrm{Coeff}^4]\le 3\,\big(\mathbb E[\mathrm{Coeff}^2]\big)^2+\sum_w p^{-3}(1-p)B_w^4.E[Coeff4]≤3(E[Coeff2])2+w∑​p−3(1−p)Bw4​.

The first term 3(E[Coeff2])2=3(σ2)23(\mathbb E[\mathrm{Coeff}^2])^2=3(\sigma^2)^23(E[Coeff2])2=3(σ2)2 is the Gaussian (Wick/pairing) leading term — the (2⋅2−1)!!=3(2\cdot2-1)!!=3(2⋅2−1)!!=3 pairings of four indices into two pairs — and σ2=E[Coeff2]=1−pp∥B∥F2\sigma^2=\mathbb E[\mathrm{Coeff}^2]=\frac{1-p}{p}\lVert B\rVert_F^2σ2=E[Coeff2]=p1−p​∥B∥F2​. The second term is the diagonal (fourth-cumulant / almost-sure) contribution ∑wE[hw4]≤∑wp−3(1−p)Bw4\sum_w\mathbb E[h_w^4]\le\sum_w p^{-3}(1-p)B_w^4∑w​E[hw4​]≤∑w​p−3(1−p)Bw4​. This is the q=4q=4q=4 case of the moment form of Bernstein's inequality (Boucheron-Lugosi-Massart, Concentration Inequalities, OUP 2013, Ch. 15; Rosenthal 1970).

Preamble
import Definitions.Def_matrix_completion_neumann
import Definitions.Def_matrix_completion_tangent
open MatrixCompletion
open scoped BigOperators Classical
Formal statement
theorem centered_sampling_coefficient_fourth_moment_bound {n₁ n₂ : ℕ} (p : ℝ) (hp0 : 0 < p) (hp1 : p ≤ 1)
    (B : Matrix (Fin n₁) (Fin n₂) ℝ) :
    bernoulliExpectation p
      (fun Omega => (matrixEntrySum (centeredSamplingFluctuation Omega p B)) ^ 4) ≤
      3 * (bernoulliExpectation p
            (fun Omega => (matrixEntrySum (centeredSamplingFluctuation Omega p B)) ^ 2)) ^ 2
      + ∑ w : Fin n₁ × Fin n₂, p⁻¹^3 * (1 - p) * (B w.1 w.2)^4 := by sorry

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