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Stationary profiles maximize entropy on their fibre

Proved
mme_stothers_general_joint_entropy_maximal

by allychan327 · Sep 8, 2026 · Mathlib 777aaa6 (Lean v4.29.0-rc3)

algebraic-complexityentropylaser-methodmatrix-multiplication

Every stationary integral profile maximizes entropy on its own marginal fibre.

Let β∗\beta^{*}β∗ be a strictly positive integral ten-class profile whose normalized version ai=βi∗/Da_i = \beta^{*}_i/Dai​=βi∗​/D satisfies the two stationarity equations of N\mathcal NN,

a3a82=a5a6a10,a4a8a9=a5a7a10a_3 a_8^2 = a_5 a_6 a_{10}, \qquad a_4 a_8 a_9 = a_5 a_7 a_{10}a3​a82​=a5​a6​a10​,a4​a8​a9​=a5​a7​a10​

(in the journal's one-based class order). Let τ\tauτ be the induced distribution on the 454545 supported ordered grade triples, i.e. τσ=ar(σ)/3\tau_\sigma = a_{r(\sigma)}/3τσ​=ar(σ)​/3 where r(σ)r(\sigma)r(σ) is the Table-1 class of σ\sigmaσ. Then for every probability distribution ρ\rhoρ on the same 454545 triples with the same three grade marginals,

H(ρ)  ≤  H(τ).H(\rho)\;\le\;H(\tau).H(ρ)≤H(τ).

No permutation symmetry is assumed of the competitor ρ\rhoρ: the comparison is over all ordered distributions on the fibre, not only class-constant ones.

The mechanism is the Gibbs variational principle. The stationarity equations say exactly that log⁡a\log aloga is an affine function of the nine-grade statistics: there are potentials λ0,…,λ8\lambda_0,\dots,\lambda_8λ0​,…,λ8​ with log⁡τσ=c+λσ1+λσ2+λσ3\log \tau_\sigma = c + \lambda_{\sigma_1} + \lambda_{\sigma_2} + \lambda_{\sigma_3}logτσ​=c+λσ1​​+λσ2​​+λσ3​​ for every supported σ\sigmaσ. Any distribution with the same marginals therefore has the same expected log-likelihood under τ\tauτ, and non-negativity of relative entropy gives H(ρ)≤H(τ)H(\rho)\le H(\tau)H(ρ)≤H(τ). The two stationarity equations are precisely the two consistency conditions that make the ten class logarithms expressible through nine potentials, one per grade.

This is the profile-parametric form of the published fixed-witness entropy maximality, and it is the input the general Theorem 5.3 chain needs: it identifies which profile controls the completion-star degree on a given marginal fibre.

Preamble
import Definitions.Def_mme_stothers_general_outer_profile
import Definitions.Def_mme_modern_entropy_data

open MME BigOperators

set_option autoImplicit false
Formal statement
theorem mme_stothers_general_joint_entropy_maximal
    (bstar : Fin 10 → ℕ) (hpos : ∀ r, 0 < bstar r)
    (hInN : MME.StothersFourth.InN (MME.StothersFourth.genProfileB bstar)) :
    let Omega :=
      {sigma : Fin 3 → Fin 9 // (∑ s, (sigma s).val) = 8}
    let target : Omega → ℝ := fun sigma ↦
      (MME.StothersFourth.genJointMultiplicity bstar 1 sigma.1 : ℝ) /
        (MME.StothersFourth.genOuterLength bstar 1 : ℝ)
    ∀ rho : Omega → ℝ,
      (∀ sigma, 0 ≤ rho sigma) →
      (∑ sigma, rho sigma) = 1 →
      (∀ s : Fin 3, ∀ j : Fin 9,
        mme_modern_marginal (fun sigma : Omega ↦ sigma.1 s) rho j =
          mme_modern_marginal
            (fun sigma : Omega ↦ sigma.1 s) target j) →
      mme_modern_entropyBits rho ≤ mme_modern_entropyBits target := by
  sorry
Source
A. M. Davie and A. J. Stothers, Improved Bound for Complexity of Matrix Multiplication, Proceedings of the Royal Society of Edinburgh A 143(2), 2013, Equation (5.2) and Lemma 5.2, with the stationarity equations of A. J. Stothers, On the Complexity of Matrix Multiplication, PhD thesis, University of Edinburgh, 2010, Chapter 4.2, pp. 78-79; https://www.maths.ed.ac.uk/~sandy/a11164.pdf.

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