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Minkowski space is a vacuum solution

Proved
EinsteinFieldEquationsD.minkowski_vacuum_solution

by Lucas · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

differential-geometryeinstein-field-equationsgeneral-relativity

The Minkowski metric η=diag⁡(−1,1,1,1)\eta=\operatorname{diag}(-1,1,1,1)η=diag(−1,1,1,1) on R4\mathbb{R}^4R4 is a smooth nondegenerate symmetric metric on all of R4\mathbb{R}^4R4, it is Ricci-flat, and it solves the vacuum field equations with zero cosmological constant (for any coupling κ\kappaκ).

Preamble
import Mathlib
import Definitions.Def_EinsteinFieldEquationsD_Defs
Formal statement
namespace EinsteinFieldEquationsD

theorem minkowski_vacuum_solution (κ : ℝ) :
    IsMetricOn minkowskiMetric Set.univ ∧
      (∀ x : Coord 4, ∀ a b : Fin 4, ricci minkowskiMetric x a b = 0) ∧
      EinsteinFieldEquationsOn minkowskiMetric 0 0 κ Set.univ := by sorry

end EinsteinFieldEquationsD
Source
Wikipedia, "Einstein field equations", revision oldid=1374672993, https://en.wikipedia.org/w/index.php?title=Einstein_field_equations&oldid=1374672993; section 'Vacuum field equations'
Read-back

What the Lean code literally says, in plain math · Aristotle (Harmonic) - same agent as the drafter; non-blind

Non-blind read-back — not independent testimony. This read-back was written by the same agent (Aristotle, by Harmonic) that drafted the Lean statements it describes, with full knowledge of the source and of the intended meaning. It is not the output of a blind, independent auditor, and no reviewer should treat it as such. Compare it against the Lean code yourself.

Here κ\kappaκ is an arbitrary real and η\etaη is the constant field on R4\mathbb{R}^4R4 whose value at every point is the diagonal matrix diag⁡(−1,1,1,1)\operatorname{diag}(-1,1,1,1)diag(−1,1,1,1).

Claim. All three of the following hold:

  1. η\etaη is a metric on R4\mathbb{R}^4R4 (the whole space is open, components are C∞C^\inftyC∞, η\etaη is symmetric and det⁡η≠0\det\eta\neq0detη=0 everywhere);
  2. for every x∈R4x\in\mathbb{R}^4x∈R4 and all a,ba,ba,b: Rab(x)=0R_{ab}(x)=0Rab​(x)=0 for the Ricci tensor of η\etaη;
  3. for every x∈R4x\in\mathbb{R}^4x∈R4 and all a,ba,ba,b: Gab(x)+0⋅ηab=κ⋅0G_{ab}(x)+0\cdot\eta_{ab}=\kappa\cdot0Gab​(x)+0⋅ηab​=κ⋅0, i.e. the field equations hold with T≡0T\equiv0T≡0 and Λ=0\Lambda=0Λ=0.
Human review
  • Endorsed by Shuze Chen · Oct 10, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Lucas · Oct 10, 2026

    Confirmed by the mission captain (proposal self-audit).

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