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Coordinate DEC along the collar for actual source fields

Proved
OAI.CKSMixedGeometry.source_actual_collar_coordinate_DEC

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

cks-bondi-penrosegeneral-relativityoai-math

Let KKK be a compact set of matrix three-jets with positive-definite values and B≥0B\ge 0B≥0. There is R0≥1R_0\ge 1R0​≥1 such that the following holds for all R≥R0R\ge R_0R≥R0​, all source tensor fields fff and all log-radius and angle pairs (ρ,x)(\rho,x)(ρ,x) with R≤eρ≤3RR\le e^\rho\le 3RR≤eρ≤3R. Assume fff is regular at the point with radius eρe^\rhoeρ and angle xxx, f.base.mK and f.base.ek are C3C^3C3 there, the source metric is positive definite nearby, the angular jet lies in KKK, and the jets of σ,mg,mK,mr\sigma,m^g,m^K,m^rσ,mg,mK,mr and the components of fff obey the bounds with constant BBB. If the coordinate DEC holds for the original data (oldParams of the collar parameters), then it holds for the collar data with parameters collarParams R (exp ρ).

So on the whole collar R≤r≤3RR\le r\le 3RR≤r≤3R the deformation by the rounding and padding weights preserves the coordinate DEC.

Formal statement. In the scope of the preamble:

theorem source_actual_collar_coordinate_DEC {K : Set MatrixThreeJet} (hK : IsCompact K)
    (hreg : ∀ q ∈ K, Matrix.PosDef (fun i k => (q i k).1.1))
    {B : ℝ} (hB : 0 ≤ B) :
    ∃ R₀ : ℝ, 1 ≤ R₀ ∧ ∀ (R : ℝ) (f : SourceTensorFields) (ρ : ℝ) (x : AP),
      R₀ ≤ R → R ≤ Real.exp ρ → Real.exp ρ ≤ 3*R →
      f.RegularAt (logRadiusChart (slice ρ x)) →
      ContDiffAt ℝ 3 f.base.mK (angularProjection (logRadiusChart (slice ρ x))) →
      ContDiffAt ℝ 3 f.base.ek (logRadiusChart (slice ρ x)) →
      (∀ᶠ y in 𝓝 (logRadiusChart (slice ρ x)), (sourceMetric f.base y).PosDef) →
      matrixThreeJets (angularLift f.base.sigma) (slice ρ x) ∈ K →
      ‖matrixThreeJets (angularLift f.base.sigma) (slice ρ x)‖ ≤ B →
      ‖matrixThreeJets (angularLift f.base.mg) (slice ρ x)‖ ≤ B →
      ‖matrixScalarJets (angularLift f.base.mK) (slice ρ x)‖ ≤ B →
      ‖actualScalarJet (angularLift f.base.mr) (slice ρ x)‖ ≤ B →
      f.ComponentBounds B (logRadiusChart (slice ρ x)) →
      CKSAngularGeometry.coordinateDEC
        (CKSAngularGeometry.fieldNullInput
          (CKSAngularGeometry.oldParams (CKSBending.collarParams R (Real.exp ρ)))
          ((sourceCollarData f.logFields).angular ρ) x) (Real.exp ρ) →
      CKSAngularGeometry.coordinateDEC
        (CKSAngularGeometry.fieldNullInput (CKSBending.collarParams R (Real.exp ρ))
          ((sourceCollarData f.logFields).angular ρ) x) (Real.exp ρ)

Formalization Note The statement is verbatim from lean/OAI/Geometry/Relativity/CKS/SourceCollarBound.lean, lines 33-64, in OpenAI's openai/math at commit adc7f12 (Apache-2.0), formalizing part of the construction in the preprint Area-controlled end replacement and the Bondi–Penrose inequality in the CKS class (OpenAI, September 27, 2026). It is a supporting lemma for OAI.CKSSourceExterior.area_controlled_end_replacement. The definitions it mentions are those of Definitions.Def_CKSBondiPenrose and Definitions.Def_CKSEndReplacementSupport.

Preamble
import Mathlib
import Definitions.Def_CKSBondiPenrose
import Definitions.Def_CKSEndReplacementSupport

namespace OAI

noncomputable section
namespace CKSMixedGeometry
noncomputable section
open CKSCalculus Set Filter Matrix CKSAngularSlice
open scoped Topology ContDiff NNReal Matrix.Norms.Elementwise

Formal statement
theorem source_actual_collar_coordinate_DEC {K : Set MatrixThreeJet} (hK : IsCompact K)
    (hreg : ∀ q ∈ K, Matrix.PosDef (fun i k => (q i k).1.1))
    {B : ℝ} (hB : 0 ≤ B) :
    ∃ R₀ : ℝ, 1 ≤ R₀ ∧ ∀ (R : ℝ) (f : SourceTensorFields) (ρ : ℝ) (x : AP),
      R₀ ≤ R → R ≤ Real.exp ρ → Real.exp ρ ≤ 3*R →
      f.RegularAt (logRadiusChart (slice ρ x)) →
      ContDiffAt ℝ 3 f.base.mK (angularProjection (logRadiusChart (slice ρ x))) →
      ContDiffAt ℝ 3 f.base.ek (logRadiusChart (slice ρ x)) →
      (∀ᶠ y in 𝓝 (logRadiusChart (slice ρ x)), (sourceMetric f.base y).PosDef) →
      matrixThreeJets (angularLift f.base.sigma) (slice ρ x) ∈ K →
      ‖matrixThreeJets (angularLift f.base.sigma) (slice ρ x)‖ ≤ B →
      ‖matrixThreeJets (angularLift f.base.mg) (slice ρ x)‖ ≤ B →
      ‖matrixScalarJets (angularLift f.base.mK) (slice ρ x)‖ ≤ B →
      ‖actualScalarJet (angularLift f.base.mr) (slice ρ x)‖ ≤ B →
      f.ComponentBounds B (logRadiusChart (slice ρ x)) →
      CKSAngularGeometry.coordinateDEC
        (CKSAngularGeometry.fieldNullInput
          (CKSAngularGeometry.oldParams (CKSBending.collarParams R (Real.exp ρ)))
          ((sourceCollarData f.logFields).angular ρ) x) (Real.exp ρ) →
      CKSAngularGeometry.coordinateDEC
        (CKSAngularGeometry.fieldNullInput (CKSBending.collarParams R (Real.exp ρ))
          ((sourceCollarData f.logFields).angular ρ) x) (Real.exp ρ) := by
  sorry

end
end CKSMixedGeometry
end
end OAI
Source
https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/lean/OAI/Geometry/Relativity/CKS/SourceCollarBound.lean#L33-L64 ; preprint preprints/Area-controlled-end-replacement-and-the-Bondi-Penrose-inequality-in-the-CKS-class-September-27-2026/paper.pdf in the same repository

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