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Every five-dimensional span(1, u, u⁻¹, QR₁/(uP), PR₂/(uQ)) with P/Q of degree 2 carries the configuration (1, P/Q) ⊗ (Q/u, R₂/u, QR₁/(uP))

Proved
DiazModulus.quadratic_two_orbit_space_carries_two_by_three_configuration

by carlok · Oct 23, 2026 · Mathlib 0df444a (Lean v4.33.1)

diaz-modulus-leannumber-theorytranscendence

Let u∈Cu \in \mathbb{C}u∈C be transcendental, that is, u∉Q‾u \notin \overline{\mathbb{Q}}u∈/Q​ (the algebraic numbers); spans and linear independence are over Q‾\overline{\mathbb{Q}}Q​. Let P,Q,R1,R2∈Q‾[X]P, Q, R_1, R_2 \in \overline{\mathbb{Q}}[X]P,Q,R1​,R2​∈Q​[X] with max⁡(deg⁡P,deg⁡Q)=2\max(\deg P, \deg Q) = 2max(degP,degQ)=2 and deg⁡R1,deg⁡R2≤2\deg R_1, \deg R_2 \leq 2degR1​,degR2​≤2, and suppose W=span(1,u,u−1,Q(u)R1(u)/(uP(u)),P(u)R2(u)/(uQ(u)))W = \mathrm{span}(1, u, u^{-1}, Q(u)R_1(u)/(uP(u)), P(u)R_2(u)/(uQ(u)))W=span(1,u,u−1,Q(u)R1​(u)/(uP(u)),P(u)R2​(u)/(uQ(u))) has dimension 555. Then x=(1,P(u)/Q(u))x = (1, P(u)/Q(u))x=(1,P(u)/Q(u)) and y=(Q(u)/u,R2(u)/u,Q(u)R1(u)/(uP(u)))y = (Q(u)/u, R_2(u)/u, Q(u)R_1(u)/(uP(u)))y=(Q(u)/u,R2​(u)/u,Q(u)R1​(u)/(uP(u))) are each linearly independent, and xiyj∈Wx_iy_j \in Wxi​yj​∈W for all i,ji, ji,j.

So every five-dimensional space of shape (D2a) carries a 2×32 \times 32×3 configuration with ratio P(u)/Q(u)P(u)/Q(u)P(u)/Q(u). PPP and QQQ need not be coprime.

Proof. Write g1=Q(u)R1(u)/(uP(u))g_1 = Q(u)R_1(u)/(uP(u))g1​=Q(u)R1​(u)/(uP(u)) and g2=P(u)R2(u)/(uQ(u))g_2 = P(u)R_2(u)/(uQ(u))g2​=P(u)R2​(u)/(uQ(u)). As WWW has dimension 555, the family 1,u,u−1,g1,g21, u, u^{-1}, g_1, g_21,u,u−1,g1​,g2​ is independent; in particular g1,g2≠0g_1, g_2 \neq 0g1​,g2​=0, so P(u),Q(u)≠0P(u), Q(u) \neq 0P(u),Q(u)=0. Every R(u)/uR(u)/uR(u)/u with deg⁡R≤2\deg R \leq 2degR≤2 lies in H0H_0H0​, so a relation R(u)/u+ag1+bg2=0R(u)/u + ag_1 + bg_2 = 0R(u)/u+ag1​+bg2​=0 forces a=b=0a = b = 0a=b=0 and R(u)=0R(u) = 0R(u)=0. The products are explicit (values at uuu): (P/Q)(Q/u)=P/u(P/Q)(Q/u) = P/u(P/Q)(Q/u)=P/u, (P/Q)(R2/u)=g2(P/Q)(R_2/u) = g_2(P/Q)(R2​/u)=g2​, (P/Q)g1=R1/u(P/Q)g_1 = R_1/u(P/Q)g1​=R1​/u, and the row 111 gives Q/u,R2/u,g1Q/u, R_2/u, g_1Q/u,R2​/u,g1​. Independence of xxx: multiplying a+bP/Q=0a + bP/Q = 0a+bP/Q=0 by R2/uR_2/uR2​/u gives aR2/u+bg2=0aR_2/u + bg_2 = 0aR2​/u+bg2​=0, so b=0b = 0b=0, then a=0a = 0a=0. Independence of yyy: the coefficient of g1g_1g1​ in a relation vanishes; multiplying the relation by P/QP/QP/Q gives (aP+cR1)/u+bg2=0(aP + cR_1)/u + bg_2 = 0(aP+cR1​)/u+bg2​=0, so b=0b = 0b=0; then aQ(u)/u=0aQ(u)/u = 0aQ(u)/u=0 gives a=0a = 0a=0. No transcendence is used beyond u≠0u \neq 0u=0.

Novelty. Not found in the sources read; routine. Explicit identities: the existence of a configuration is the easy direction; the classification is Theorem NF (DiazModulus.degree_two_configuration_normal_form).

Preamble
import Definitions.Def_DiazModulus
Formal statement
open Complex ComplexConjugate

namespace DiazModulus

open Polynomial in
theorem quadratic_two_orbit_space_carries_two_by_three_configuration (u : ℂ) (hu : u ∉ Qbar)
    (P Q R₁ R₂ : (↥Qbar)[X]) (hdeg : max P.natDegree Q.natDegree = 2)
    (hR₁ : R₁.natDegree ≤ 2) (hR₂ : R₂.natDegree ≤ 2)
    (h5 : Module.finrank (↥Qbar) (Submodule.span Qbar ({1, u, u⁻¹, aeval u Q * aeval u R₁ / (u * aeval u P),
        aeval u P * aeval u R₂ / (u * aeval u Q)} : Set ℂ)) = 5) :
    LinearIndependent (↥Qbar) ![1, aeval u P / aeval u Q] ∧
    LinearIndependent (↥Qbar) ![aeval u Q / u, aeval u R₂ / u, aeval u Q * aeval u R₁ / (u * aeval u P)] ∧
    ∀ i j, ![1, aeval u P / aeval u Q] i *
      ![aeval u Q / u, aeval u R₂ / u, aeval u Q * aeval u R₁ / (u * aeval u P)] j ∈
      Submodule.span Qbar ({1, u, u⁻¹, aeval u Q * aeval u R₁ / (u * aeval u P),
        aeval u P * aeval u R₂ / (u * aeval u Q)} : Set ℂ) := by
  sorry

end DiazModulus
Source
Not found in the sources read. The space is the two-orbit normal form of the mission's research notes (round R12, Q1.3), there in the coordinate h − c. R20 of the Diaz modulus mission. Formal proof: Diaz modulus mission, 23 October 2026 (C. Perassi).

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