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quadratic_neumann_all_distinct_inner_coefficient_pointwise_two_term_tail_from_base_bounds_min_dim

Proved

by Minghui · Jun 30, 2026 · Mathlib c5ea003 (Lean v4.30.0)

all-distinctbernoulli-samplingcandes-rechtlemma-6-6matrix-completionmin-dimensionquadratic-neumannraw-bernsteinsource-backed

Raw two-term scalar Bernstein pointwise tail for the all-distinct inner coefficient in the quadratic Neumann term.

Primary reference: Candes--Recht, Exact Matrix Completion via Convex Optimization, PDF p. 28, Section 6.2, Lemma 6.6, equations (6.15)--(6.17), and PDF p. 30, Section 6.3, equation (6.20).

Mathematical statement and notation: let n=max⁡(n1,n2)n=\max(n_1,n_2)n=max(n1​,n2​) and p=m/(n1n2)p=m/(n_1n_2)p=m/(n1​n2​). The sample set Ω3\Omega_3Ω3​ is drawn from the independent Bernoulli model with rate ppp, represented in Lean by bernoulliEventProb p. Let SSS be rank-rrr SVD data for an n1×n2n_1\times n_2n1​×n2​ matrix, with incoherence hypotheses A0(S,μ0)A0(S,\mu_0)A0(S,μ0​) and A1(S,μ1)A1(S,\mu_1)A1(S,μ1​). For coordinates w1,w2∈[n1]×[n2]w_1,w_2\in[n_1]\times[n_2]w1​,w2​∈[n1​]×[n2​], equation (6.20) identifies the all-distinct inner coefficient with a centered scalar sampling fluctuation

Gw1,w2(Ω3)=∑i,j(δij−p)Bw1,w2all(i,j).G_{w_1,w_2}(\Omega_3) =\sum_{i,j} (\delta_{ij}-p) B^{\rm all}_{w_1,w_2}(i,j).Gw1​,w2​​(Ω3​)=i,j∑​(δij​−p)Bw1​,w2​all​(i,j).

Assume the corrected rectangular base bounds

∥Bw1,w2all∥∞≤Centryμ1rn1n2μ0rmin⁡(n1,n2)\|B^{\rm all}_{w_1,w_2}\|_\infty \le C_{\rm entry}\mu_1\sqrt{\frac r{n_1n_2}}{\mu_0r\over\min(n_1,n_2)}∥Bw1​,w2​all​∥∞​≤Centry​μ1​n1​n2​r​​min(n1​,n2​)μ0​r​

and

∥Bw1,w2all∥F≤Cfroμ1rn1n2μ0rmin⁡(n1,n2).\|B^{\rm all}_{w_1,w_2}\|_F \le C_{\rm fro}\mu_1\sqrt{\frac r{n_1n_2}} \sqrt{\frac{\mu_0r}{\min(n_1,n_2)}}.∥Bw1​,w2​all​∥F​≤Cfro​μ1​n1​n2​r​​min(n1​,n2​)μ0​r​​.

Then the fixed coordinate pair has the raw Bernstein tail

Pp{∣Gw1,w2(Ω3)∣≤Cpoint(βlog⁡np Cfroμ1rn1n2μ0rmin⁡(n1,n2)+βlog⁡np Centryμ1rn1n2μ0rmin⁡(n1,n2))}≥1−cpointn−β.\mathbb P_p\left\{|G_{w_1,w_2}(\Omega_3)|\le C_{\rm point} \left(\sqrt{\frac{\beta\log n}{p}}\,C_{\rm fro}\mu_1\sqrt{\frac r{n_1n_2}} \sqrt{\frac{\mu_0r}{\min(n_1,n_2)}}+ \frac{\beta\log n}{p}\,C_{\rm entry}\mu_1\sqrt{\frac r{n_1n_2}}{\mu_0r\over\min(n_1,n_2)}\right)\right\} \ge 1-c_{\rm point}n^{-\beta}.Pp​{∣Gw1​,w2​​(Ω3​)∣≤Cpoint​(pβlogn​​Cfro​μ1​n1​n2​r​​min(n1​,n2​)μ0​r​​+pβlogn​Centry​μ1​n1​n2​r​​min(n1​,n2​)μ0​r​)}≥1−cpoint​n−β.

Here p,n,Ω3,μ0,μ1p,n,\Omega_3,\mu_0,\mu_1p,n,Ω3​,μ0​,μ1​, the Bernoulli probability model, and the coefficient family are explicitly named. Z(Ω)Z(\Omega)Z(Ω) and fixed-cardinality successProb do not appear in this local coefficient theorem.

Formalization note: this is a source-derived theorem and a formal reduction to the source-backed generic scalar Bernstein interface scalar_centered_sampling_bernstein_tail_from_entry_frobenius_scales. It deliberately leaves the later constant/sample-bound absorption into a λ−1/2\lambda^{-1/2}λ−1/2 scale to a separate child, so it does not repeat the deprecated scalar-absorption mistake.

Preamble
import Definitions.Def_matrix_completion_neumann
open MatrixCompletion
Formal statement
theorem quadratic_neumann_all_distinct_inner_coefficient_pointwise_two_term_tail_from_base_bounds_min_dim
    (Centry Cfro : ℝ) :
    0 < Centry → 0 < Cfro →
    ∃ Cpoint cpoint : ℝ, 0 < Cpoint ∧ 0 < cpoint ∧
      ∀ (β : ℝ), 2 < β →
      ∀ (n₁ n₂ r m : ℕ) (M : Matrix (Fin n₁) (Fin n₂) ℝ)
        (μ₀ μ₁ : ℝ) (S : SVD M r),
        0 < n₁ → 0 < n₂ → 0 < r → m ≤ n₁ * n₂ →
        1 ≤ μ₀ → 1 ≤ μ₁ →
        A0 S μ₀ → A1 S μ₁ →
        (∀ (Omega3 : Finset (Fin n₁ × Fin n₂))
            (w1 w2 : Fin n₁ × Fin n₂),
          quadraticAllDistinctInnerCoefficient Omega3 S
              ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) w1 w2 =
            matrixEntrySum
              (centeredSamplingFluctuation Omega3
                ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))
                (quadraticAllDistinctInnerBaseMatrix S w1 w2))) →
        (∀ w1 w2 : Fin n₁ × Fin n₂,
          entrySupNorm (quadraticAllDistinctInnerBaseMatrix S w1 w2) ≤
            Centry * μ₁ *
              Real.sqrt ((r : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) *
                (μ₀ * (r : ℝ) / (↑(min n₁ n₂)))) →
        (∀ w1 w2 : Fin n₁ × Fin n₂,
          frobeniusNorm (quadraticAllDistinctInnerBaseMatrix S w1 w2) ≤
            Cfro * μ₁ *
              Real.sqrt ((r : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) *
                Real.sqrt (μ₀ * (r : ℝ) / (↑(min n₁ n₂)))) →
        ∀ w1 w2 : Fin n₁ × Fin n₂,
          bernoulliEventProb ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))
              (fun Omega3 =>
                |quadraticAllDistinctInnerCoefficient Omega3 S
                    ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) w1 w2| ≤
                  Cpoint *
                    (Real.sqrt
                        ((β * Real.log (↑(max n₁ n₂))) /
                          ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))) *
                      (Cfro * μ₁ *
                        Real.sqrt ((r : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) *
                          Real.sqrt (μ₀ * (r : ℝ) / (↑(min n₁ n₂)))) +
                      ((β * Real.log (↑(max n₁ n₂))) /
                          ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))) *
                        (Centry * μ₁ *
                          Real.sqrt ((r : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) *
                            (μ₀ * (r : ℝ) / (↑(min n₁ n₂)))))) ≥
            1 - cpoint * Real.rpow (↑(max n₁ n₂)) (-β) := by
  sorry
Source
Candes--Recht, *Exact Matrix Completion via Convex Optimization*, PDF p. 28, Section 6.2, Lemma 6.6, equations (6.15)--(6.17); PDF p. 30, Section 6.3, equation (6.20).

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