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For the same u, a₁, a₂, W = Q̄ + Q̄u + Q̄ū + Q̄u/(u² − a₁) + Q̄u/(u² − a₂) carries a 2×3 configuration, while no Q̄ + Q̄u + Q̄ū + Q̄w with w ∈ W outside Q̄ + Q̄u + Q̄ū does

Proved
DiazModulus.circle_point_two_pole_configuration_invisible_to_four_dimensional_extensions

by carlok · Oct 9, 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​ with ρ=uuˉ\rho = u\bar uρ=uuˉ algebraic, let a1≠a2a_1 \neq a_2a1​=a2​ be non-zero algebraic numbers, zi=u/(u2−ai)z_i = u/(u^2 - a_i)zi​=u/(u2−ai​), H0=Q‾+Q‾u+Q‾uˉH_0 = \overline{\mathbb{Q}} + \overline{\mathbb{Q}}u + \overline{\mathbb{Q}}\bar uH0​=Q​+Q​u+Q​uˉ and W=H0+Q‾z1+Q‾z2W = H_0 + \overline{\mathbb{Q}}z_1 + \overline{\mathbb{Q}}z_2W=H0​+Q​z1​+Q​z2​. Then WWW carries a 2×32 \times 32×3 configuration, but for no w∈Ww \in Ww∈W outside H0H_0H0​ does H0+Q‾wH_0 + \overline{\mathbb{Q}}wH0​+Q​w carry one.

This removes the conjugation condition from DiazModulus.circle_point_conjugate_pair_configuration_invisible_to_four_dimensional_extensions (the case a2=ρ2/aˉ1a_2 = \rho^2/\bar a_1a2​=ρ2/aˉ1​), and covers the case a1aˉ1=a2aˉ2=ρ2a_1\bar a_1 = a_2\bar a_2 = \rho^2a1​aˉ1​=a2​aˉ2​=ρ2, where WWW is stable under conjugation.

Proof. The configuration is DiazModulus.circle_point_two_pole_extension_carries_two_by_three_configuration. If w∈W∖H0w \in W \setminus H_0w∈W∖H0​ and H0+Q‾wH_0 + \overline{\mathbb{Q}}wH0​+Q​w carried one, Theorem B (DiazModulus.circle_point_extension_two_by_three_configuration_iff) would give w∈H0+Q‾tw \in H_0 + \overline{\mathbb{Q}}tw∈H0​+Q​t with ttt one of u2u^2u2, uˉ2\bar u^2uˉ2, 1/(u−b)1/(u - b)1/(u−b) (bbb algebraic, non-zero); exchange then puts ttt in H0+Q‾w⊆WH_0 + \overline{\mathbb{Q}}w \subseteq WH0​+Q​w⊆W, which DiazModulus.circle_point_two_pole_extension_excludes_squares_and_reciprocals rules out.

Novelty. Not found in the sources read; it is short (parity plus Theorem B).

Preamble
import Definitions.Def_DiazModulus
Formal statement
open Complex ComplexConjugate

namespace DiazModulus

theorem circle_point_two_pole_configuration_invisible_to_four_dimensional_extensions (u a₁ a₂ : ℂ)
    (hu : u ∉ Qbar) (hρ : IsAlgebraic ℚ (u * conj u)) (ha₁ : a₁ ∈ Qbar) (ha₂ : a₂ ∈ Qbar)
    (ha₁0 : a₁ ≠ 0) (ha₂0 : a₂ ≠ 0) (ha : a₁ ≠ a₂) :
    (∃ (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, u / (u ^ 2 - a₁), u / (u ^ 2 - a₂)} : Set ℂ)) ∧
      ∀ w ∈ Submodule.span Qbar ({1, u, conj u, u / (u ^ 2 - a₁), u / (u ^ 2 - a₂)} : 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; the configuration's shape is printed (S. Fischler, Orbits under algebraic groups and logarithms of algebraic numbers, Acta Arith. 100 (2001), 167–187, Lemma 6.1). Uses DiazModulus.circle_point_extension_two_by_three_configuration_iff (Theorem B of the Diaz modulus mission). R7 of the Diaz modulus mission. Formal proof: Diaz modulus mission, 9 October 2026 (C. Perassi).

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