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Prop. 2.1 (G3): curvature conditions after Trautman geometrization

Proved
NewtonCartan.geometrization_curvConds

by Ethan Cheung Wang · Oct 21, 2026 · Mathlib 0df444a (Lean v4.33.1)

classical-spacetimecurvaturegeometrized-newtonian-gravitationnewton-cartan

Let (R4,ta,hab,∇)(\mathbb R^4,t_a,h^{ab},\nabla)(R4,ta​,hab,∇) be a flat classical spacetime and let smooth φ,ρ\varphi,\rhoφ,ρ satisfy Poisson's equation ∇a∇aφ=4πρ\nabla^a\nabla_a\varphi=4\pi\rho∇a∇a​φ=4πρ. Write ∇~=(∇,−tbtc∇aφ)\tilde\nabla=(\nabla,-t_bt_c\nabla^a\varphi)∇~=(∇,−tb​tc​∇aφ) for the Trautman geometrization. Then the curvature of ∇~\tilde\nabla∇~ satisfies (1) Rab=4πρtatbR_{ab}=4\pi\rho t_a t_bRab​=4πρta​tb​, (2) Rabcd=RcdabR^a{}_b{}^c{}_d=R^c{}_d{}^a{}_bRab​cd​=Rcd​ab​, and (3) Rabcd=0R^{ab}{}_{cd}=0Rabcd​=0.

Preamble
import Definitions.Def_NewtonCartan_defs

open scoped ContDiff
Formal statement
namespace NewtonCartan

/-- Curvature conditions of Prop. 2.1 / Malament 4.2.1 (G3): after Trautman geometrization,
`(1) R_{ab}=4πρ t_a t_b`, `(2) R^a{}_b{}^c{}_d=R^c{}_d{}^a{}_b`, `(3) R^{ab}{}_{cd}=0`. -/
theorem geometrization_curvConds (Γ : Conn) (φ ρ : E → ℝ) (hNG : IsNG Γ φ)
    (hρ : ContDiff ℝ ∞ ρ) (hP : Poisson Γ φ ρ) :
    CurvConds (geomΓ Γ φ) ρ := by sorry

end NewtonCartan
Source
J. O. Weatherall, arXiv:1411.5757, Prop. 2.1 curvature conditions (1)–(3) (p. 4); D. B. Malament, Topics… (2012), Prop. 4.2.1 (G3), eqs. (4.2.4)–(4.2.6)

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