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Standard Schwarzschild metric is the pull-back of the Eddington–Finkelstein metric

Proved
ExactVacuumAtlas.Schwarzschild.EFRelation.pullback

by He Wang · Oct 13, 2026 · Mathlib 0df444a (Lean v4.33.1)

coordinate-geometrycoordinate-transformationeddington-finkelsteinexact-vacuum-atlasgeneral-relativityschwarzschild-metric

Let M,εM,\varepsilonM,ε be real numbers with ε2=1\varepsilon^2=1ε2=1 and x=(t,r,θ,φ)∈UMstd={r>0, r≠2M, 0<θ<π}x=(t,r,\theta,\varphi)\in U^{\rm std}_M=\{r>0,\ r\neq2M,\ 0<\theta<\pi\}x=(t,r,θ,φ)∈UMstd​={r>0, r=2M, 0<θ<π}. Let ΦM,ε(t,r,θ,φ)=(t+ε(r+2Mlog⁡∣r−2M∣),r,θ,φ)\Phi_{M,\varepsilon}(t,r,\theta,\varphi)=(t+\varepsilon(r+2M\log\lvert r-2M\rvert),r,\theta,\varphi)ΦM,ε​(t,r,θ,φ)=(t+ε(r+2Mlog∣r−2M∣),r,θ,φ) and

J(x)=(1ε(1+2Mr−2M)00010000100001).J(x)=\begin{pmatrix}1&\varepsilon\big(1+\frac{2M}{r-2M}\big)&0&0\\0&1&0&0\\0&0&1&0\\0&0&0&1\end{pmatrix}.J(x)=​1000​ε(1+r−2M2M​)100​0010​0001​​.

Then, with gMstdg^{\rm std}_MgMstd​ the standard Schwarzschild metric gMstdg^{\rm std}_MgMstd​ (bundle Atlas_Schwarzschild_Defs, coordinates (t,r,θ,φ)(t,r,\theta,\varphi)(t,r,θ,φ)): gtt=−(1−2M/r)g_{tt}=-(1-2M/r)gtt​=−(1−2M/r), grr=1/(1−2M/r)g_{rr}=1/(1-2M/r)grr​=1/(1−2M/r), gθθ=r2g_{\theta\theta}=r^2gθθ​=r2, gφφ=r2sin⁡2θg_{\varphi\varphi}=r^2\sin^2\thetagφφ​=r2sin2θ, other entries 000, with candidate inverse g^tt=−1/(1−2M/r)\hat g^{tt}=-1/(1-2M/r)g^​tt=−1/(1−2M/r), g^rr=1−2M/r\hat g^{rr}=1-2M/rg^​rr=1−2M/r, g^θθ=1/r2\hat g^{\theta\theta}=1/r^2g^​θθ=1/r2, g^φφ=1/(r2sin⁡2θ)\hat g^{\varphi\varphi}=1/(r^2\sin^2\theta)g^​φφ=1/(r2sin2θ) and gM,εEFg^{\rm EF}_{M,\varepsilon}gM,εEF​ the Eddington–Finkelstein family gM,εEFg^{\rm EF}_{M,\varepsilon}gM,εEF​ (bundle Atlas_Schwarzschild_Defs, coordinates (w,r,θ,φ)(w,r,\theta,\varphi)(w,r,θ,φ) with w=vw=vw=v for ε=1\varepsilon=1ε=1 ingoing and w=uw=uw=u for ε=−1\varepsilon=-1ε=−1 outgoing): gww=−(1−2M/r)g_{ww}=-(1-2M/r)gww​=−(1−2M/r), gwr=grw=εg_{wr}=g_{rw}=\varepsilongwr​=grw​=ε, gθθ=r2g_{\theta\theta}=r^2gθθ​=r2, gφφ=r2sin⁡2θg_{\varphi\varphi}=r^2\sin^2\thetagφφ​=r2sin2θ, other entries 000, with candidate inverse g^wr=g^rw=ε\hat g^{wr}=\hat g^{rw}=\varepsilong^​wr=g^​rw=ε, g^rr=1−2M/r\hat g^{rr}=1-2M/rg^​rr=1−2M/r, g^θθ=1/r2\hat g^{\theta\theta}=1/r^2g^​θθ=1/r2, g^φφ=1/(r2sin⁡2θ)\hat g^{\varphi\varphi}=1/(r^2\sin^2\theta)g^​φφ=1/(r2sin2θ), other entries 000:

J(x)T gM,εEF(ΦM,ε(x)) J(x)=gMstd(x).J(x)^{\mathsf T}\,g^{\rm EF}_{M,\varepsilon}\big(\Phi_{M,\varepsilon}(x)\big)\,J(x)=g^{\rm std}_M(x).J(x)TgM,εEF​(ΦM,ε​(x))J(x)=gMstd​(x).

Pull-back obligation of relations R1 (ε=1\varepsilon=1ε=1) and R2 (ε=−1\varepsilon=-1ε=−1); det⁡J=1\det J=1detJ=1.

Formalization Note Everything is coordinate-level on R4\mathbb R^4R4 (points are functions {0,1,2,3}→R\{0,1,2,3\}\to\mathbb R{0,1,2,3}→R): no manifold, chart gluing, periodicity of φ\varphiφ, horizon, causal or global statement is made. Partial derivatives are Mathlib's deriv of coordinate slices; the certificates' C∞C^\inftyC∞ obligations make every derivative used a genuine derivative. Units G=c=1G=c=1G=c=1, signature (−,+,+,+)(-,+,+,+)(−,+,+,+).

Formalization Note (logarithm). log⁡∣r−2M∣\log\lvert r-2M\rvertlog∣r−2M∣ stands for Mathlib's Real.log (r - 2M), which equals log⁡∣r−2M∣\log\lvert r-2M\rvertlog∣r−2M∣ for every r≠2Mr\neq2Mr=2M (Real.log_abs); the Lean expression is unchanged and the domain is not restricted to r>2Mr>2Mr>2M.

Preamble
import Mathlib
import Definitions.Def_Atlas_Core_Basic
import Definitions.Def_Atlas_Core_Lift
import Definitions.Def_Atlas_Schwarzschild_Defs
import Definitions.Def_Atlas_Schwarzschild_Domain
import Definitions.Def_Atlas_Schwarzschild_EFCertParts
import Definitions.Def_Atlas_Schwarzschild_EFRelation
import Definitions.Def_Atlas_Schwarzschild_StdParts
import Definitions.Def_KerrBL_CoordGeometry
import Definitions.Def_KerrBL_Kerr_Metric
open Real
open ExactVacuumAtlas ExactVacuumAtlas.Schwarzschild
open ExactVacuumAtlas
open ExactVacuumAtlas.Schwarzschild
open ExactVacuumAtlas.Schwarzschild.EFRelation
set_option maxHeartbeats 4000000
Formal statement
theorem ExactVacuumAtlas.Schwarzschild.EFRelation.pullback (M ε : ℝ) (hε : ε ^ 2 = 1) {x : Pt 4} (hx : x ∈ domStd M) :
    (jac M ε x).transpose * metricMatrix (gEF M ε) (toEF M ε x) * jac M ε x =
      metricMatrix (gStd M) x := by sorry
Source
Müller–Grave catalogue eq. eddFinkel: ds² = −(1−r_s/r) dv² + 2 dv dr + r² dΩ², v = t + r + r_s ln(r − r_s); outgoing form with u = t − r − r_s ln|r − r_s|; Müller–Grave catalogue eq. schwarzschildSpherical (r_s = 2M, G = c = 1); Lean source: repository ExactVacuumAtlas (private repository, not publicly accessible; GitHub remote pending (no GitHub identity on the build server)), commit 35f26e6a22f5d72380094fa94edc72dea667df53, Atlas/Schwarzschild/EFPullback.lean#L21-L37 (module Atlas.Schwarzschild.EFPullback, file sha256 f6efed4d3c5874ace673dbcb0f3074b4377453f13641565322c9a762e06eee33; uploaded stub = platform_mirror/Theorems/Thm_ExactVacuumAtlas_Schwarzschild_EFRelation_pullback.lean)
Human review
  • Endorsed by Shuze Chen · Oct 14, 2026

    Confirmed by the moderator at approval.

  • Endorsed by He Wang · Oct 14, 2026

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

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