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quadratic_neumann_all_distinct_inner_coefficients_from_base_bounds_min_dim_shifted

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

all-distinctbernoulli-samplingcandes-rechtformal-bridgelemma-6-6matrix-completionmin-dimensionquadratic-neumannsource-backed

Formal bridge from the corrected min-dimension pointwise all-distinct inner coefficient tail to the simultaneous coefficient event with the required ordered-pair union-bound shift.

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

Mathematical statement and notation: set 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 event is over the Bernoulli sample Ω3\Omega_3Ω3​ with probability bernoulliEventProb p. For SVD data SSS satisfying A0(S,μ0)A0(S,\mu_0)A0(S,μ0​) and A1(S,μ1)A1(S,\mu_1)A1(S,μ1​), equation (6.20) identifies each all-distinct inner coefficient as

Gw1,w2(Ω3)=∑i,j(1(i,j)∈Ω3−p)Bw1,w2all(i,j).G_{w_1,w_2}(\Omega_3) = \sum_{i,j}(1_{(i,j)\in\Omega_3}-p)B^{\rm all}_{w_1,w_2}(i,j).Gw1​,w2​​(Ω3​)=i,j∑​(1(i,j)∈Ω3​​−p)Bw1​,w2​all​(i,j).

Assume the corrected min-dimension entry and Frobenius bounds for Bw1,w2allB^{\rm all}_{w_1,w_2}Bw1​,w2​all​ and the sample lower bound both at exponent β\betaβ and at shifted exponent β+4\beta+4β+4:

m≥λμ04/3nr4/3βlog⁡n,m≥λμ04/3nr4/3(β+4)log⁡n.m\ge \lambda\mu_0^{4/3}n r^{4/3}\beta\log n, \qquad m\ge \lambda\mu_0^{4/3}n r^{4/3}(\beta+4)\log n.m≥λμ04/3​nr4/3βlogn,m≥λμ04/3​nr4/3(β+4)logn.

Then, after applying the pointwise child at exponent β+4\beta+4β+4 and paying the ordered-pair union-bound cost (n1n2)2≤n4(n_1n_2)^2\le n^4(n1​n2​)2≤n4, the simultaneous event holds:

Pp{∀w1,w2,∣Gw1,w2(Ω3)∣≤Cinnerλ−1/2}≥1−cinnern−β.\mathbb P_p\{\forall w_1,w_2, |G_{w_1,w_2}(\Omega_3)|\le C_{\rm inner}\lambda^{-1/2}\} \ge 1-c_{\rm inner}n^{-\beta}.Pp​{∀w1​,w2​,∣Gw1​,w2​​(Ω3​)∣≤Cinner​λ−1/2}≥1−cinner​n−β.

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

Formalization note: this is a formal bridge, not a theorem appearing verbatim in the paper. It should import the source-backed pointwise child quadratic_neumann_all_distinct_inner_coefficient_pointwise_tail_from_base_bounds_min_dim and the already proved source-backed uniformization child quadratic_neumann_all_distinct_inner_coefficients_uniform_from_shifted_pointwise_tails (c325fcc3-f5e1-48f4-acdb-12c7ae7ea619). The bridge replaces the stale old route through quadratic_neumann_all_distinct_inner_coefficients_from_base_bounds, whose accepted sketch uses the deprecated unshifted uniformization child.

Preamble
import Definitions.Def_matrix_completion_neumann
open MatrixCompletion
Formal statement
theorem quadratic_neumann_all_distinct_inner_coefficients_from_base_bounds_min_dim_shifted
    (Centry Cfro : ℝ) :
    0 < Centry → 0 < Cfro →
    ∃ Cinner cinner : ℝ, 0 < Cinner ∧ 0 < cinner ∧
      ∀ (β lam : ℝ), 2 < β → 1 ≤ lam →
      ∀ (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 →
        (m : ℝ) ≥
          lam * Real.rpow μ₀ ((4 : ℝ) / 3) *
            (↑(max n₁ n₂)) * Real.rpow (r : ℝ) ((4 : ℝ) / 3) *
              (β * Real.log (↑(max n₁ n₂))) →
        (m : ℝ) ≥
          lam * Real.rpow μ₀ ((4 : ℝ) / 3) *
            (↑(max n₁ n₂)) * Real.rpow (r : ℝ) ((4 : ℝ) / 3) *
              ((β + 4) * Real.log (↑(max n₁ n₂))) →
        (∀ (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)))) →
        bernoulliEventProb ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))
            (fun Omega3 =>
              QuadraticAllDistinctInnerCoefficientBound Omega3 S
                ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))
                (Cinner * Real.rpow lam (-((1 : ℝ) / 2)))) ≥
          1 - cinner * Real.rpow (↑(max n₁ n₂)) (-β) := by
  sorry
Source
Formal bridge. Source-backed analytic child: 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). The ordered-pair union-bound child is the proved source-backed theorem `quadratic_neumann_all_distinct_inner_coefficients_uniform_from_shifted_pointwise_tails`.

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