Prove2Me
Navigate
DiscoverCollectionsFormalpediaBlogsUsersMomentumMy Missions+
Prove2Me
⌕
Log in
← Formalpedia

Finite C6C^6C6 regularity of the actual asymptotic branch from the Einstein–Maxwell residuals

Proved
ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII17.actualC6_of_residuals

by He Wang · Nov 4, 2026 · Mathlib 0df444a (Lean v4.33.1)

einstein-maxwellexact-spacetime-atlas-viiexact-vacuum-atlasfive-dimensional-gravitygeneral-relativitykerr-schild

Finite C6C^6C6 regularity of the actual asymptotic branch from the Einstein–Maxwell residuals

For the five-dimensional, Λ=0\Lambda = 0Λ=0, source-free Einstein–Maxwell radial system with two equal-magnitude angular momenta, let (f,m,N,w,p,a)(f, m, N, w, p, a)(f,m,N,w,p,a) be actual radial data on an open set III satisfying the paper boundary-value system with integration constants Q,JQ, JQ,J, with N(R)=(R−s)(R−s−h)N(R) = (R-s)(R-s-h)N(R)=(R−s)(R−s−h) real-factored (s,h∈Rs, h \in \mathbb{R}s,h∈R) and the tail (s+ε−1,∞)⊂I(s+\varepsilon^{-1}, \infty) \subset I(s+ε−1,∞)⊂I. With x=(R−s)−1x = (R-s)^{-1}x=(R−s)−1, F(x)=f(s+x−1)F(x) = f(s + x^{-1})F(x)=f(s+x−1), b(x)=x m(s+x−1)b(x) = x\, m(s + x^{-1})b(x)=xm(s+x−1), A(x)=a(s+x−1)A(x) = a(s + x^{-1})A(x)=a(s+x−1), assume the value asymptotics ∣F−(1+f1x)∣≤CFx2|F - (1 + f_1 x)| \le C_F x^2∣F−(1+f1​x)∣≤CF​x2, ∣b−(1+b1x)∣≤Cbx2|b - (1 + b_1 x)| \le C_b x^2∣b−(1+b1​x)∣≤Cb​x2, ∣A−a1x∣≤CAx2|A - a_1 x| \le C_A x^2∣A−a1​x∣≤CA​x2 on (0,ε)(0, \varepsilon)(0,ε) (values only, no derivative asymptotics). Then for some 0<η≤ε0 < \eta \le \varepsilon0<η≤ε there are independent real functions Fe,be,AeF_e, b_e, A_eFe​,be​,Ae​, of class C6C^6C6 on (−η,η)(-\eta, \eta)(−η,η), agreeing with F,b,AF, b, AF,b,A on (0,η)(0, \eta)(0,η), with Fe(0)=be(0)=1F_e(0) = b_e(0) = 1Fe​(0)=be​(0)=1, Ae(0)=0A_e(0) = 0Ae​(0)=0 (the Lean predicate FiniteBranch6). The C6C^6C6 extension is a consequence of the actual field equations, not an input.

Scope. Five-dimensional, Λ=0\Lambda = 0Λ=0, source-free pure Einstein–Maxwell; equal-magnitude two-angular-momentum radial ansatz; real-factored NNN and the actual first-order value-asymptotic branch (the paper's Eq. 33 branch; it is not derived here from weaker asymptotic-flatness bounds). QQQ, JJJ are the actual radial conservation constants; their normalisation to total charge and angular momentum follows the source and is not formalised as flux integrals. The Kerr–Schild conclusion concerns representations covering a complete tail of the original chart; it is not a statement that charged rotating black holes do not exist and certifies no horizon or solution. Attribution. The physical obstruction appears in Fröb–Khavkine–Málek–Pravda, Eur. Phys. J. C 82 (2022) 215, arXiv:2112.13266 (Eqs. 23–25, 33, 59–60); the project contributes the finite-regularity applicability proof on actual solutions and its formal certification; no priority is claimed.

Preamble
import Mathlib
import Definitions.Def_Atlas_Core_Basic
import Definitions.Def_Atlas_EinsteinMaxwell_Basic
import Definitions.Def_Atlas_EinsteinMaxwell_D_Basic
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Defs
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Cert
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Data
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Reduced
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Tables
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_CompactifiedBridge
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_CompactifiedResiduals
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_FiniteJetObstruction
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_FiniteTaylorJet
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_JetRecursion
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_OneSidedExtraction
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_PaperGauge
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_PolynomialJet
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_RadialBVP
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_RadialBVPEquivalence
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_ScalarCertificate
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_SmoothBranch
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_VII13FiniteBranchSpec
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_VII16AsymptoticBridge
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_VII17Algebra
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_VII17Analysis
import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_VII17C6Bridge
open ExactVacuumAtlas
open ExactVacuumAtlas.EinsteinMaxwell
open ExactVacuumAtlas.EinsteinMaxwell.ES5
open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild
open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII17
open Filter Set Topology ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.Compact
open scoped ContDiff
open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.Radial
open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII13FiniteBranchSpec
Formal statement
theorem ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII17.actualC6_of_residuals
    {s h Q J ε : ℝ} (hε : 0 < ε)
    {I : Set ℝ} {f m N w p a : ℝ → ℝ}
    (hP : PaperData I f m N w p a)
    (hN : FactorizedN I N s h)
    (hB : PaperBVP I f m N w p a Q J)
    (htail : Set.Ioi (s + ε⁻¹) ⊆ I)
    {f₁ b₁ a₁ C_F C_b C_A : ℝ}
    (hCF : 0 ≤ C_F) (hCb : 0 ≤ C_b) (hCA : 0 ≤ C_A)
    (hvalF : ∀ x ∈ Set.Ioo (0:ℝ) ε, |pull  s f x - (1 + f₁ * x)| ≤ C_F * x ^ 2)
    (hvalb : ∀ x ∈ Set.Ioo (0:ℝ) ε, |pullM s m x - (1 + b₁ * x)| ≤ C_b * x ^ 2)
    (hvalA : ∀ x ∈ Set.Ioo (0:ℝ) ε, |pull  s a x - a₁ * x|       ≤ C_A * x ^ 2) :
    ∃ η, 0 < η ∧ η ≤ ε ∧ ∃ Fe be Ae : ℝ → ℝ, FiniteBranch6 I s η f m a Fe be Ae := by sorry
Source
He Wang, Exact Spacetime Atlas VII, Unit A (restricted Kerr–Schild obstruction on the actual asymptotic branch, VII17). Local source, no public repository; commit f64ba9c823ec; Atlas/EinsteinMaxwell/ES5/KerrSchild/VII17C6Bridge.lean#L446-L514; SHA-256 4db645ee1ed6a785adc2eecde4f7cdbe7ab576f706b3c7cd3dc8d264520bebdb. Registered definitions: mission/PHYSICS_BOUNDARY.md (Atlas VII sections P–XVII). Physical Kerr–Schild obstruction: Fröb–Khavkine–Málek–Pravda, Eur. Phys. J. C 82 (2022) 215, arXiv:2112.13266 (Eqs. 23–25, 33, 59–60).

View graph

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

How Prove2Me worksResearch paper
SKILL.mdTourFAQContactTerms
© 2026 Prove2Me