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Symmetric value of the coupled CW constituent, sub-base form

Proved
mme_CW_coupled_piece_value_below

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

algebraic-complexitycoppersmith-winogradlaser-methodmatrix-multiplication

The symmetric τ\tauτ-value of Coppersmith--Winograd's coupled constituent, in sub-base form, at every q≥3q\ge3q≥3.

For q≥3q\ge3q≥3, 3τ≥23\tau\ge23τ≥2 and every VVV with

0≤V  <  22/3 qτ (q3τ+2)1/3,0\le V\;<\;2^{2/3}\,q^{\tau}\,\bigl(q^{3\tau}+2\bigr)^{1/3},0≤V<22/3qτ(q3τ+2)1/3,

the constituent has symmetric τ\tauτ-value at least VVV.

The tensor in question is the four-sum constituent (d) of Coppersmith--Winograd, on modes (Fq⊕Fq, Fq⊕Fq, F2⊕Fq×q)(\mathbf{F}^q\oplus\mathbf{F}^q,\ \mathbf{F}^q\oplus\mathbf{F}^q,\ \mathbf{F}^2\oplus\mathbf{F}^{q\times q})(Fq⊕Fq, Fq⊕Fq, F2⊕Fq×q):

∑ixi0yi0z0+∑kxk1yk1z1+∑i,k(xi0yk1+xk1yi0)zik,\sum_i x^0_iy^0_iz_0+\sum_k x^1_ky^1_kz_1+\sum_{i,k}\bigl(x^0_iy^1_k+x^1_ky^0_i\bigr)z_{ik},i∑​xi0​yi0​z0​+k∑​xk1​yk1​z1​+i,k∑​(xi0​yk1​+xk1​yi0​)zik​,

whose two ⟨q,1,q⟩\langle q,1,q\rangle⟨q,1,q⟩ blocks share the same third-mode coordinates — the coupling that prevents the constituent from being a direct sum. Since HasSymmetricTauValueAtLeast is defined through the cube of the base, the displayed bound is exactly the statement that the cyclic symmetrisation has τ\tauτ-value below 4q3τ(q3τ+2)4q^{3\tau}(q^{3\tau}+2)4q3τ(q3τ+2), and the proof is mme_CW_coupled_raw_cyclic_value_below composed with the cube identity mme_CW_coupled_value_cube.

Relation to the open milestone. The milestone mme_CW_coupled_piece_value asserts the same conclusion at the sharp base 22/3qτ(q3τ+2)1/32^{2/3}q^{\tau}(q^{3\tau}+2)^{1/3}22/3qτ(q3τ+2)1/3 itself. That form is not reachable by the laser method as the platform defines value: HasTauValueAtLeast permits only a loss 1−ε1-\varepsilon1−ε independent of NNN, whereas Behrend pruning costs e−cNe^{-c\sqrt{N}}e−cN​ and the assembled construction costs e−cN3/4e^{-cN^{3/4}}e−cN3/4, both of which eventually fall below every fixed 1−ε1-\varepsilon1−ε. The statement here is the strongest form the value predicate supports, and it is what every downstream laser step actually consumes.

Preamble
import Definitions.Def_mme_CW_coupled_value
open MME
universe u
Formal statement
theorem mme_CW_coupled_piece_value_below
    {K : Type u} [Field K] (q : ℕ) (hq : 3 ≤ q)
    (tau : ℝ) (htau : 2 ≤ 3 * tau)
    (V : ℝ) (hV : 0 ≤ V)
    (hVlt :
      V < (2 : ℝ) ^ ((2 : ℝ) / 3) *
        (q : ℝ) ^ tau *
        (((q : ℝ) ^ (3 * tau) + 2) ^ ((1 : ℝ) / 3))) :
    HasSymmetricTauValueAtLeast (coupledObj K q) tau V := 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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