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Even-power extraction from the coupled constituent at every q

Proved
mme_CW_coupled_tensor_extraction_below_raw

by allychan327 · Sep 7, 2026 · Mathlib 777aaa6 (Lean v4.29.0-rc3)

algebraic-complexitycoppersmith-winogradlaser-methodmatrix-multiplication

Finite extraction from even powers of the coupled constituent, at every q≥3q\ge3q≥3.

Let q≥3q\ge3q≥3, 3τ≥23\tau\ge23τ≥2, and let 0≤V<raw=4q3τ(q3τ+2)0\le V<\mathrm{raw}=4q^{3\tau}(q^{3\tau}+2)0≤V<raw=4q3τ(q3τ+2). Then eventually in NNN, on the floor profile satisfying the pruning conditions, the 2N2N2N-th Kronecker power of the cyclic symmetrisation of the coupled constituent restricts from a direct sum of kkk matrix-multiplication tensors with

V2N  ≤  ∑i(aibici)τ.V^{2N}\;\le\;\sum_i (a_ib_ic_i)^{\tau}.V2N≤i∑​(ai​bi​ci​)τ.

The proof multiplies three ingredients: the capacity estimate mme_CW_primary_profile_capacity_quarter_root, the hash certificates mme_CW_primary_hash_Ctensor_outer_middle_certificates, and the quarter-root absorption mme_MM_induced_matching_quarter_root_absorption that converts the Behrend loss e−100log⁡He^{-100\sqrt{\log H}}e−100logH​ into the uniform quarter-root loss. Every surviving star contributes the same volume (q4G+2L)3\bigl(q^{4G+2L}\bigr)^3(q4G+2L)3, so the weighted sum collapses to k⋅(side3)τk\cdot(\text{side}^3)^\tauk⋅(side3)τ and the estimate becomes the capacity inequality.

The strict inequality V<rawV<\mathrm{raw}V<raw is what makes the argument work: it gives V≤raw⋅e−lossV\le \mathrm{raw}\cdot e^{-\text{loss}}V≤raw⋅e−loss for all large NNN, and the two factors of e−N losse^{-N\,\text{loss}}e−Nloss that this produces are exactly what pay for the hashing and Behrend losses.

General-qqq form of mme_CW_q6_coupled_tensor_extraction_below_raw_of_pruning, with the pruning conditions supplied as a hypothesis.

Preamble
import Mathlib.Analysis.SpecificLimits.Basic
import Definitions.Def_mme_CW_coupled_value
open MME BigOperators Filter
universe u
Formal statement
theorem mme_CW_coupled_tensor_extraction_below_raw
    {K : Type u} [Field K] (q : ℕ) (hq : 3 ≤ q)
    (tau : ℝ) (htau : 2 ≤ 3 * tau)
    (V : ℝ) (hV : 0 ≤ V)
    (hVlt :
      V < 4 * (q : ℝ) ^ (3 * tau) *
        ((q : ℝ) ^ (3 * tau) + 2)) :
    ∀ᶠ N : ℕ in atTop,
      let lambda : ℝ := 2 / ((q : ℝ) ^ (3 * tau) + 2)
      let L : ℕ := ⌊lambda * (N : ℝ)⌋₊
      let G : ℕ := N - L
      (0 < L ∧ 0 < G ∧ L + G = N ∧ 341 * L < 100 * G) →
      ∃ (k : ℕ) (a b c : Fin k → ℕ),
        TensorObj.Restrict
          (TensorObj.bigAdd (fun i => MMObj K (a i) (b i) (c i)))
          ((cyclicSymmetrization (coupledObj K q)).kronPow (2 * N)) ∧
        V ^ (2 * N) ≤
          ∑ i, (((a i * b i * c i : ℕ) : ℝ) ^ tau) := by
  sorry
Source
Don Coppersmith and Shmuel Winograd, Matrix multiplication via arithmetic progressions, Journal of Symbolic Computation 9(3), 1990, 251-280; the coupled four-sum constituent (d) on printed p. 266 and its value lemma on printed p. 270. General-q form of the q=6 chain used for omega < 2.376.

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