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quadratic_neumann_all_distinct_inner_base_norms_le_linear_offdiag_base

Proved

by Minghui · Jun 26, 2026 · Mathlib c5ea003 (Lean v4.30.0)

candes-rechtexact-matrix-completionformal-bridgelean4neumann-seriessource-backed

Source: Candès--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: For rank-rrr SVD data SSS of M∈Rn1×n2M\in\mathbb R^{n_1\times n_2}M∈Rn1​×n2​ and coordinates w1,w2∈[n1]×[n2]w_1,w_2\in [n_1]\times[n_2]w1​,w2​∈[n1​]×[n2​], let

Bw1,w2all(i,j)={0,(i,j)=w1 or (i,j)=w2,sgn⁡(S)ij KS((i,j),w2),otherwise,B^{\mathrm{all}}_{w_1,w_2}(i,j) =\begin{cases} 0, & (i,j)=w_1\text{ or }(i,j)=w_2,\\ \operatorname{sgn}(S)_{ij}\,K_S((i,j),w_2), & \text{otherwise}, \end{cases}Bw1​,w2​all​(i,j)={0,sgn(S)ij​KS​((i,j),w2​),​(i,j)=w1​ or (i,j)=w2​,otherwise,​

be the all-distinct inner base matrix from the equation (6.20) branch. Let

Bw2lin(i,j)={0,(i,j)=w2,sgn⁡(S)ij KS((i,j),w2),otherwise,B^{\mathrm{lin}}_{w_2}(i,j) =\begin{cases} 0, & (i,j)=w_2,\\ \operatorname{sgn}(S)_{ij}\,K_S((i,j),w_2), & \text{otherwise}, \end{cases}Bw2​lin​(i,j)={0,sgn(S)ij​KS​((i,j),w2​),​(i,j)=w2​,otherwise,​

be the linear off-diagonal Lemma 6.6 base matrix. Then the extra zeroing at w1w_1w1​ cannot increase either deterministic norm:

∥Bw1,w2all∥∞≤∥Bw2lin∥∞,∥Bw1,w2all∥F≤∥Bw2lin∥F.\|B^{\mathrm{all}}_{w_1,w_2}\|_\infty \le \|B^{\mathrm{lin}}_{w_2}\|_\infty, \qquad \|B^{\mathrm{all}}_{w_1,w_2}\|_F \le \|B^{\mathrm{lin}}_{w_2}\|_F.∥Bw1​,w2​all​∥∞​≤∥Bw2​lin​∥∞​,∥Bw1​,w2​all​∥F​≤∥Bw2​lin​∥F​.

Notation context: Here n=max⁡(n1,n2)n=\max(n_1,n_2)n=max(n1​,n2​) is downstream matrix-completion notation, although it is not needed by this deterministic bridge. The Bernoulli rate p=m/(n1n2)p=m/(n_1n_2)p=m/(n1​n2​) and sample set Ω\OmegaΩ are downstream in Lemma 6.6 and equation (6.20), but do not appear in this norm comparison. The coherence parameters μ0\mu_0μ0​ and μ1\mu_1μ1​ are used by the source-backed parent base-bound theorems, not by this zeroing bridge. Z(Ω)Z(\Omega)Z(Ω) does not appear.

Formalization note: This is a formal bridge, not a theorem stated verbatim in the paper. It connects the all-distinct equation (6.20) base matrix to the source-backed linear off-diagonal Lemma 6.6 base matrix by pointwise zeroing. The intended source-backed parent/import theorems are linear_neumann_off_diagonal_coefficient_base_entry_sup_norm_bound_min_dim and linear_neumann_off_diagonal_coefficient_base_frobenius_norm_bound_min_dim, whose source is Candès--Recht PDF p. 28, Section 6.2, Lemma 6.6, equations (6.15)--(6.17). This bridge is useful before deriving corrected all-distinct min-dimension base bounds, and it deliberately avoids the disproved old max-denominator all-distinct base-bound nodes.

Preamble
import Definitions.Def_linear_neumann_offdiag_bernstein
open MatrixCompletion
open scoped Classical BigOperators
Formal statement
theorem quadratic_neumann_all_distinct_inner_base_norms_le_linear_offdiag_base
    {n₁ n₂ r : Nat} {M : Matrix (Fin n₁) (Fin n₂) ℝ}
    (S : SVD M r) (w1 w2 : Fin n₁ × Fin n₂) :
    entrySupNorm (quadraticAllDistinctInnerBaseMatrix S w1 w2) ≤
        entrySupNorm (linearNeumannOffDiagonalCoefficientBaseMatrix S w2) ∧
      frobeniusNorm (quadraticAllDistinctInnerBaseMatrix S w1 w2) ≤
        frobeniusNorm (linearNeumannOffDiagonalCoefficientBaseMatrix S w2) := by
  sorry
Source
Candès--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).

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