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For u ∉ Q̄ and real algebraic s with s² = uū, the cyclic space with double poles at ±s carries no 2×3 configuration whose ratio is a Möbius function of u

Proved
DiazModulus.cyclic_pair_space_no_mobius_ratio_configuration

by carlok · Oct 15, 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​ and let s∈Q‾s \in \overline{\mathbb{Q}}s∈Q​ be real with s2=uuˉs^2 = u\bar us2=uuˉ (so uˉ=s2/u\bar u = s^2/uuˉ=s2/u). With v=u/sv = u/sv=u/s, put G1=1/(v−1)+2/(v+1)G_1 = 1/(v - 1) + 2/(v + 1)G1​=1/(v−1)+2/(v+1) and G2=1/(v−1)2+1/(v−1)−2/(v+1)2+2/(v+1)G_2 = 1/(v - 1)^2 + 1/(v - 1) - 2/(v + 1)^2 + 2/(v + 1)G2​=1/(v−1)2+1/(v−1)−2/(v+1)2+2/(v+1), and let WWW be the Q‾\overline{\mathbb{Q}}Q​-span of 1,u,uˉ,G1,G21, u, \bar u, G_1, G_21,u,uˉ,G1​,G2​ (poles at u=±su = \pm su=±s, each a double pole). Then there are no free x1,x2x_1, x_2x1​,x2​ and free y1,y2,y3y_1, y_2, y_3y1​,y2​,y3​ with all six products in WWW and x2/x1=(αu+β)/(γu+δ)x_2/x_1 = (\alpha u + \beta)/(\gamma u + \delta)x2​/x1​=(αu+β)/(γu+δ), α,β,γ,δ∈Q‾\alpha, \beta, \gamma, \delta \in \overline{\mathbb{Q}}α,β,γ,δ∈Q​, αδ−βγ≠0\alpha\delta - \beta\gamma \neq 0αδ−βγ=0.

So, like R14's W1W_1W1​, it is none of R11's real pencil spaces.

Proof. First, if ttt and ututut both lie in WWW, then t∈Q‾+Q‾uˉt \in \overline{\mathbb{Q}} + \overline{\mathbb{Q}}\bar ut∈Q​+Q​uˉ. Write t=c1+c2u+c3uˉ+c4G1+c5G2t = c_1 + c_2u + c_3\bar u + c_4G_1 + c_5G_2t=c1​+c2​u+c3​uˉ+c4​G1​+c5​G2​, and ututut likewise, and multiply each by u(u2−s2)2u(u^2 - s^2)^2u(u2−s2)2, which turns them into polynomials of degree 666 in uuu (as in DiazModulus.cyclic_pair_space_excludes_squares_and_reciprocals). Then u⋅u(u2−s2)2t=u(u2−s2)2⋅utu \cdot u(u^2 - s^2)^2t = u(u^2 - s^2)^2 \cdot utu⋅u(u2−s2)2t=u(u2−s2)2⋅ut is an identity of degree 777 over Q‾\overline{\mathbb{Q}}Q​ at the transcendental uuu. Its u7u^7u7 coefficient gives c2=0c_2 = 0c2​=0, and two combinations of the eight coefficient equations give 16s6c4=016s^6c_4 = 016s6c4​=0 and 16s6c5=016s^6c_5 = 016s6c5​=0. (In terms of poles: in WWW the leading polar coefficients at sss and −s-s−s are in the ratio 1:−21 : -21:−2 for double poles and 1:21 : 21:2 for simple ones, and multiplication by uuu changes the sign of that ratio.) Now let free xxx and yyy have xiyj∈Wx_iy_j \in Wxi​yj​∈W and x2(γu+δ)=x1(αu+β)x_2(\gamma u + \delta) = x_1(\alpha u + \beta)x2​(γu+δ)=x1​(αu+β) with αδ−βγ≠0\alpha\delta - \beta\gamma \neq 0αδ−βγ=0. Then c=αx1−γx2≠0c = \alpha x_1 - \gamma x_2 \neq 0c=αx1​−γx2​=0 by the freeness of xxx, the three numbers tj=cyjt_j = cy_jtj​=cyj​ are free and lie in WWW, and utj=δx2yj−βx1yj∈Wut_j = \delta x_2y_j - \beta x_1y_j \in Wutj​=δx2​yj​−βx1​yj​∈W. So three free numbers lie in the two-dimensional Q‾+Q‾uˉ\overline{\mathbb{Q}} + \overline{\mathbb{Q}}\bar uQ​+Q​uˉ, which is impossible.

Novelty. Not found in the sources read; routine.

Preamble
import Definitions.Def_DiazModulus
Formal statement
open Complex ComplexConjugate

namespace DiazModulus

theorem cyclic_pair_space_no_mobius_ratio_configuration
    (u s : ℂ) (hu : u ∉ Qbar) (hs : s ∈ Qbar) (hsr : conj s = s) (hss : s * s = u * conj u) :
    ¬ ∃ (x : Fin 2 → ℂ) (y : Fin 3 → ℂ) (α β γ δ : ℂ), α ∈ Qbar ∧ β ∈ Qbar ∧ γ ∈ Qbar ∧ δ ∈ Qbar ∧
      α * δ - β * γ ≠ 0 ∧ LinearIndependent (↥Qbar) x ∧ LinearIndependent (↥Qbar) y ∧
      (∀ i j, x i * y j ∈ Submodule.span Qbar ({1, u, conj u, (s / (u - s) + 2 * s / (u + s)), (s * s / (u - s) ^ 2 + s / (u - s) - 2 * (s * s) / (u + s) ^ 2 + 2 * s / (u + s))} : Set ℂ)) ∧ x 1 * (γ * u + δ) = x 0 * (α * u + β) := by
  sorry

end DiazModulus
Source
Not found in the sources read. R15 of the Diaz modulus mission. Formal proof: Diaz modulus mission, 15 October 2026 (C. Perassi).

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