quadratic_neumann_all_distinct_inner_coefficient_pointwise_tail_from_structural_a0_min_dim
OpenStructural A0-based 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. 6, Section 1.2, Definition 1.2 and the paragraph before Theorem 1.3, with Theorem 1.3 equation (1.9), where the paper notes that holds with by Cauchy--Schwarz; PDF p. 28, Section 6.2, Lemma 6.6, equations (6.15)--(6.17), for the scalar Bernstein coordinate bound; and PDF p. 30, Section 6.3, equation (6.20), for the all-distinct inner coefficient representation.
Mathematical statement and notation: let and . The sample set is drawn from the independent Bernoulli model with rate , represented in Lean by bernoulliEventProb p. Let be rank- SVD data for an matrix satisfying ; the statement also carries the ambient hypothesis used by surrounding nodes, but the intended structural route uses the Candes--Recht Cauchy--Schwarz consequence instead of the possibly loose input .
For coordinates , equation (6.20) identifies the all-distinct inner coefficient with a centered scalar sampling fluctuation
Under the Lemma 6.6 density floor
the theorem asserts the fixed-coordinate pointwise tail
Here , , , and the Bernoulli probability model are explicit. and fixed-cardinality successProb do not appear in this local coefficient theorem.
Formalization note: this is a source-derived structural child, not a theorem stated verbatim in the paper and not a purely formal Lean bridge. It is meant to replace a direct absorption from the raw two-term theorem using the loose input . A proof should combine the source-backed raw scalar Bernstein child quadratic_neumann_all_distinct_inner_coefficient_pointwise_two_term_tail_from_base_bounds_min_dim, the Candes--Recht Cauchy--Schwarz step, the corrected all-distinct min-dimension base-bound suppliers, and scalar absorption under the displayed density floor.
import Definitions.Def_matrix_completion_neumann open MatrixCompletion
theorem quadratic_neumann_all_distinct_inner_coefficient_pointwise_tail_from_structural_a0_min_dim :
∃ Cpoint cpoint : ℝ, 0 < Cpoint ∧ 0 < cpoint ∧
∀ (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))) →
(∀ (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,
bernoulliEventProb ((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ)))
(fun Omega3 =>
|quadraticAllDistinctInnerCoefficient Omega3 S
((m : ℝ) / ((n₁ : ℝ) * (n₂ : ℝ))) w1 w2| ≤
Cpoint * Real.rpow lam (-((1 : ℝ) / 2))) ≥
1 - cpoint * Real.rpow (↑(max n₁ n₂)) (-β) := by
sorry