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Every 2×2 matrix over Q̄ is scalar, has two distinct eigenvalues with an eigenbasis, or has a Jordan basis

Proved
DiazModulus.qbar_matrix_fin_two_eigen_or_jordan

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

diaz-modulus-leannumber-theorytranscendence

Let MMM be a 2×22 \times 22×2 matrix with entries in the field Q‾\overline{\mathbb{Q}}Q​ of algebraic numbers in C\mathbb{C}C, acting on column vectors in Q‾2\overline{\mathbb{Q}}^2Q​2. Then one of the following holds:

  • M=cIM = cIM=cI for some c∈Q‾c \in \overline{\mathbb{Q}}c∈Q​;
  • there are linearly independent v,w∈Q‾2v, w \in \overline{\mathbb{Q}}^2v,w∈Q​2 and c1≠c2c_1 \neq c_2c1​=c2​ in Q‾\overline{\mathbb{Q}}Q​ with Mv=c1vMv = c_1vMv=c1​v and Mw=c2wMw = c_2wMw=c2​w;
  • there are linearly independent v,w∈Q‾2v, w \in \overline{\mathbb{Q}}^2v,w∈Q​2 and c∈Q‾c \in \overline{\mathbb{Q}}c∈Q​ with Mv=cvMv = cvMv=cv and Mw=cw+vMw = cw + vMw=cw+v.

Proof. Write MMM with rows (a,b)(a, b)(a,b) and (c,d)(c, d)(c,d); two vectors (x,y)(x, y)(x,y), (x′,y′)(x', y')(x′,y′) are linearly independent as soon as xy′−yx′≠0xy' - yx' \neq 0xy′−yx′=0. If b=c=0b = c = 0b=c=0: when a=da = da=d, M=aIM = aIM=aI; otherwise (1,0)(1, 0)(1,0) and (0,1)(0, 1)(0,1) are eigenvectors for a≠da \neq da=d. If b=0b = 0b=0 and c≠0c \neq 0c=0: when a=da = da=d, v=(0,c)v = (0, c)v=(0,c) and w=(1,0)w = (1, 0)w=(1,0) satisfy Mv=avMv = avMv=av and Mw=aw+vMw = aw + vMw=aw+v; otherwise (0,1)(0, 1)(0,1) and (a−d,c)(a - d, c)(a−d,c) are eigenvectors for ddd and aaa. If b≠0b \neq 0b=0, take a root l∈Q‾l \in \overline{\mathbb{Q}}l∈Q​ of t2−(a+d)t+(ad−bc)t^2 - (a + d)t + (ad - bc)t2−(a+d)t+(ad−bc): a complex square root sss of the discriminant is algebraic over Q\mathbb{Q}Q, as its square is, so s∈Q‾s \in \overline{\mathbb{Q}}s∈Q​ and l=(a+d+s)/2l = (a + d + s)/2l=(a+d+s)/2. The other root is m=a+d−lm = a + d - lm=a+d−l. If l≠ml \neq ml=m, (b,l−a)(b, l - a)(b,l−a) and (b,m−a)(b, m - a)(b,m−a) are eigenvectors for lll and mmm, with determinant b(m−l)≠0b(m - l) \neq 0b(m−l)=0; if l=ml = ml=m, v=(b,l−a)v = (b, l - a)v=(b,l−a) and w=(0,1)w = (0, 1)w=(0,1) satisfy Mv=lvMv = lvMv=lv and Mw=lw+vMw = lw + vMw=lw+v. No algebraic-closedness instance for Q‾\overline{\mathbb{Q}}Q​ is used.

Novelty. Standard linear algebra; routine.

Preamble
import Definitions.Def_DiazModulus
Formal statement
open Complex ComplexConjugate

namespace DiazModulus

theorem qbar_matrix_fin_two_eigen_or_jordan (M : Matrix (Fin 2) (Fin 2) ↥Qbar) :
    (∃ c : ↥Qbar, M = c • (1 : Matrix (Fin 2) (Fin 2) ↥Qbar)) ∨
    (∃ (v w : Fin 2 → ↥Qbar) (c₁ c₂ : ↥Qbar), c₁ ≠ c₂ ∧ LinearIndependent (↥Qbar) ![v, w] ∧
        M.mulVec v = c₁ • v ∧ M.mulVec w = c₂ • w) ∨
    (∃ (v w : Fin 2 → ↥Qbar) (c : ↥Qbar), LinearIndependent (↥Qbar) ![v, w] ∧
        M.mulVec v = c • v ∧ M.mulVec w = c • w + v) := by
  sorry

end DiazModulus
Source
Standard linear algebra: the Jordan form of a 2×2 matrix over an algebraically closed field. R20 of the Diaz modulus mission. Formal proof: Diaz modulus mission, 23 October 2026 (C. Perassi).

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