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For u ∉ Q̄ with uū algebraic and the two-orbit space of a, b, α, β, γ, δ with α ≠ β or γ ≠ δ: a spanning 2×3 configuration that no Q̄ + Q̄u + Q̄ū + Q̄w inside it carries

Proved
DiazModulus.two_orbit_configuration_invisible_to_four_dimensional_extensions

by carlok · Oct 14, 2026 · Mathlib 0df444a (Lean v4.33.1)

diaz-modulus-leannumber-theorytranscendence

Let u∈C∖Q‾u \in \mathbb{C} \setminus \overline{\mathbb{Q}}u∈C∖Q​, let a,b∈Q‾×a, b \in \overline{\mathbb{Q}}^\timesa,b∈Q​× with a2≠b2a^2 \neq b^2a2=b2 and α,β,γ,δ∈Q‾×\alpha, \beta, \gamma, \delta \in \overline{\mathbb{Q}}^\timesα,β,γ,δ∈Q​×, put g1=α/(u−a)+β/(u+a)g_1 = \alpha/(u - a) + \beta/(u + a)g1​=α/(u−a)+β/(u+a), g2=γ/(u−b)+δ/(u+b)g_2 = \gamma/(u - b) + \delta/(u + b)g2​=γ/(u−b)+δ/(u+b), and let WWW be the Q‾\overline{\mathbb{Q}}Q​-span of 1,u,u−1,g1,g21, u, u^{-1}, g_1, g_21,u,u−1,g1​,g2​. Suppose α≠β\alpha \neq \betaα=β or γ≠δ\gamma \neq \deltaγ=δ, and that uuˉu\bar uuuˉ is algebraic; put H0=Q‾+Q‾u+Q‾uˉH_0 = \overline{\mathbb{Q}} + \overline{\mathbb{Q}}u + \overline{\mathbb{Q}}\bar uH0​=Q​+Q​u+Q​uˉ. Then the six products of (1,u2)(1, u^2)(1,u2) and (u−1,g1,g2)(u^{-1}, g_1, g_2)(u−1,g1​,g2​) lie in WWW and span it, and for no w∈Ww \in Ww∈W outside H0H_0H0​ does H0+Q‾wH_0 + \overline{\mathbb{Q}}wH0​+Q​w carry a configuration.

For α=β\alpha = \betaα=β, γ=δ\gamma = \deltaγ=δ the space is R7's two-pole family, whose configuration is a progression; here the products span the whole space.

Proof. With x=(1,u2)x = (1, u^2)x=(1,u2) and y=(u−1,g1,g2)y = (u^{-1}, g_1, g_2)y=(u−1,g1​,g2​): u2/(u∓a)=u±a+a2/(u∓a)u^2/(u \mp a) = u \pm a + a^2/(u \mp a)u2/(u∓a)=u±a+a2/(u∓a) gives u2g1=(α+β)u+(α−β)a+a2g1u^2g_1 = (\alpha+\beta)u + (\alpha-\beta)a + a^2g_1u2g1​=(α+β)u+(α−β)a+a2g1​, and likewise for g2g_2g2​, so the six products lie in WWW; their span contains 111 because (α−β)a(\alpha-\beta)a(α−β)a or (γ−δ)b(\gamma-\delta)b(γ−δ)b is non-zero, hence equals WWW. xxx is free since u2∉Q‾u^2 \notin \overline{\mathbb{Q}}u2∈/Q​, and yyy by DiazModulus.two_orbit_space_excludes_squares_and_reciprocals. Since uˉ=ρu−1\bar u = \rho u^{-1}uˉ=ρu−1, every H0+Q‾wH_0 + \overline{\mathbb{Q}}wH0​+Q​w with w∈Ww \in Ww∈W lies in WWW, and Theorem B (DiazModulus.circle_point_extension_two_by_three_configuration_iff) with exchange would put u2u^2u2, uˉ2\bar u^2uˉ2 (so u−2u^{-2}u−2) or some 1/(u−e)1/(u - e)1/(u−e) in WWW, which the same node excludes.

Novelty. Not found in the sources read; it is short.

Preamble
import Definitions.Def_DiazModulus
Formal statement
open Complex ComplexConjugate

namespace DiazModulus

theorem two_orbit_configuration_invisible_to_four_dimensional_extensions
    (u : ℂ) (hu : u ∉ Qbar) (a b α β γ δ : ℂ) (ha : a ∈ Qbar) (hb : b ∈ Qbar) (hα : α ∈ Qbar) (hβ : β ∈ Qbar)
    (hγ : γ ∈ Qbar) (hδ : δ ∈ Qbar) (ha0 : a ≠ 0) (hb0 : b ≠ 0) (hab : a ^ 2 ≠ b ^ 2)
    (hα0 : α ≠ 0) (hβ0 : β ≠ 0) (hγ0 : γ ≠ 0) (hδ0 : δ ≠ 0)
    (hαγ : α ≠ β ∨ γ ≠ δ) (hρ : IsAlgebraic ℚ (u * conj u)) :
    (∃ (x : Fin 2 → ℂ) (y : Fin 3 → ℂ), LinearIndependent (↥Qbar) x ∧ LinearIndependent (↥Qbar) y ∧
        (∀ i j, x i * y j ∈ Submodule.span Qbar ({1, u, u⁻¹, (α / (u - a) + β / (u + a)), (γ / (u - b) + δ / (u + b))} : Set ℂ)) ∧
        Submodule.span Qbar (Set.range (fun p : Fin 2 × Fin 3 => x p.1 * y p.2)) = Submodule.span Qbar ({1, u, u⁻¹, (α / (u - a) + β / (u + a)), (γ / (u - b) + δ / (u + b))} : Set ℂ)) ∧
      ∀ w ∈ Submodule.span Qbar ({1, u, u⁻¹, (α / (u - a) + β / (u + a)), (γ / (u - b) + δ / (u + b))} : Set ℂ), w ∉ Submodule.span Qbar ({1, u, conj u} : Set ℂ) →
        ¬ ∃ (x : Fin 2 → ℂ) (y : Fin 3 → ℂ), LinearIndependent (↥Qbar) x ∧ LinearIndependent (↥Qbar) y ∧
          ∀ i j, x i * y j ∈ Submodule.span Qbar ({1, u, conj u, w} : Set ℂ) := by
  sorry

end DiazModulus
Source
Not found in the sources read. Uses DiazModulus.circle_point_extension_two_by_three_configuration_iff (Theorem B of the Diaz modulus mission). R14 of the Diaz modulus mission. Formal proof: Diaz modulus mission, 14 October 2026 (C. Perassi).

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