Prop. 2.2: Trautman recovery
ProvedNewtonCartan.recoverySpacetime is in a global chart (index 0 = time) with , ; a derivative operator is a smooth symmetric Christoffel field ; curvature in Malament's convention , ; is the geometrization; timelike curves have unit tangent . If is a classical spacetime satisfying (1)-(3) for some smooth , there are a smooth and a flat compatible such that the timelike geodesics of are exactly the curves with , and .
import Definitions.Def_NewtonCartan_defs open scoped ContDiff
namespace NewtonCartan
/-- **Prop. 2.2 (Trautman).** Let `(ℝ⁴, t_a, h^{ab}, ∇̃)` be a classical spacetime satisfying
conditions (1)–(3) of Prop. 2.1 for some smooth `ρ`. Then there are a smooth `φ` and a flat derivative
operator `∇` such that `(ℝ⁴, t_a, h^{ab}, ∇)` is a classical spacetime, the timelike geodesics of `∇̃`
are exactly the curves with `ξ^n ∇_n ξ^a = -∇^a φ`, and `∇, φ` satisfy Poisson's equation. -/
theorem recovery (Γt : Conn) (ρ : E → ℝ) (hΓt : IsClassical Γt) (hρ : ContDiff ℝ ∞ ρ)
(hcurv : CurvConds Γt ρ) :
∃ (Γ : Conn) (φ : E → ℝ), IsNG Γ φ ∧ SameTrajectories Γ φ Γt ∧ Poisson Γ φ ρ := by sorry
end NewtonCartanRead-back
What the Lean code literally says, in plain math · claude-opus-5-5
For every classical and every with CurvConds(), there exist a connection and function with classical and flat, , SameTrajectories(), and everywhere.
Flags: hypotheses satisfiable (). -smoothness is redundant (follows from (1)). The true statement needs contractibility of (Trautman/Malament 4.2.x); a genuinely hard existence theorem, no hypotheses appear missing. No uniqueness asserted.
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.