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If K-independent x₁, x₂ and y₁, y₂ have products spanning a 3-dimensional K-space, then span(x) = K·a + K·ah and span(y) = K·b + K·bh for one h ∉ K

Proved
DiazModulus.two_by_two_config_critical_progression

by carlok · Oct 8, 2026 · Mathlib 0df444a (Lean v4.33.1)

diaz-modulus-leanlinear-algebratranscendence

Let KKK be a subfield of C\mathbb{C}C, and let x1,x2x_1, x_2x1​,x2​ and y1,y2y_1, y_2y1​,y2​ be complex numbers, each pair linearly independent over KKK, such that the four products xiyjx_iy_jxi​yj​ span a KKK-space of dimension 333. Then there are h∉Kh \notin Kh∈/K and non-zero a,ba, ba,b with span⁡K(x1,x2)=Ka+Kah\operatorname{span}_K(x_1, x_2) = Ka + KahspanK​(x1​,x2​)=Ka+Kah and span⁡K(y1,y2)=Kb+Kbh\operatorname{span}_K(y_1, y_2) = Kb + KbhspanK​(y1​,y2​)=Kb+Kbh; the products span the three-term progression ab (K+Kh+Kh2)ab\,(K + Kh + Kh^2)ab(K+Kh+Kh2).

The certificate (1,u)⊗(1,uˉ)(1, u) \otimes (1, \bar u)(1,u)⊗(1,uˉ) of a point of a circle is of this kind, with h=uh = uh=u.

Proof. Four vectors in a space of dimension 333 are dependent, so x1u′+x2v=0x_1u' + x_2v = 0x1​u′+x2​v=0 with u′=g11y1+g12y2u' = g_{11}y_1 + g_{12}y_2u′=g11​y1​+g12​y2​, v=g21y1+g22y2v = g_{21}y_1 + g_{22}y_2v=g21​y1​+g22​y2​ and g≠0g \neq 0g=0; then v≠0v \neq 0v=0. Put h=x2/x1∉Kh = x_2/x_1 \notin Kh=x2​/x1​∈/K, a=x1a = x_1a=x1​, b=vb = vb=v; then bh=−u′bh = -u'bh=−u′, the pair v,−u′v, -u'v,−u′ is independent (a relation sv−tu′=0sv - tu' = 0sv−tu′=0 gives v(sx1+tx2)=0v(sx_1 + tx_2) = 0v(sx1​+tx2​)=0), and it spans the same 222-dimensional space as y1,y2y_1, y_2y1​,y2​.

Novelty. Known in general: the dimension-2 case of Bachoc, Serra and Zémor (2017), Lemmas 4–5 (there for KKK algebraically closed in the ambient field), and of their linear Vosper theorem (Th. 33) over algebraically closed fields. Here over any subfield of C\mathbb{C}C. Not claimed.

Preamble
import Definitions.Def_DiazModulus
Formal statement
open Complex ComplexConjugate

namespace DiazModulus

theorem two_by_two_config_critical_progression (K : Subfield ℂ) (x y : Fin 2 → ℂ)
    (hx : LinearIndependent K x) (hy : LinearIndependent K y)
    (h3 : Module.finrank K
      (Submodule.span K (Set.range fun ij : Fin 2 × Fin 2 => x ij.1 * y ij.2)) = 3) :
    ∃ h a b : ℂ, h ∉ K ∧ a ≠ 0 ∧ b ≠ 0 ∧
      Submodule.span K (Set.range x) = Submodule.span K {a, a * h} ∧
      Submodule.span K (Set.range y) = Submodule.span K {b, b * h} := by
  sorry

end DiazModulus
Source
The dimension-2 case of C. Bachoc, O. Serra, G. Zémor, An analogue of Vosper's theorem for extension fields, Math. Proc. Cambridge Philos. Soc. (2017), arXiv:1501.00602, Lemmas 4–5 (stated there for a base field algebraically closed in the extension). R6 of the Diaz modulus mission (the polar-degree note). Formal proof: Diaz modulus mission, 8 October 2026 (C. Perassi).

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