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ddθ Σ(r,cos⁡θ)=−2a2sin⁡θcos⁡θ\frac{d}{d\theta}\,\Sigma(r,\cos\theta) = -2a^2\sin\theta\cos\thetadθd​Σ(r,cosθ)=−2a2sinθcosθ

Proved
KerrBL.hasDerivAt_Sig_th

by He Wang · Sep 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

coordinate-geometrygeneral-relativitykerr-metrickerrbl-missionricci-flatness

For all real a,r,θa,r,\thetaa,r,θ the function θ↦Σ(a,r,cos⁡θ)=r2+a2cos⁡2θ\theta\mapsto\Sigma(a,r,\cos\theta)=r^2+a^2\cos^2\thetaθ↦Σ(a,r,cosθ)=r2+a2cos2θ has derivative

−2 sin⁡θ cos⁡θ a2-2\,\sin\theta\,\cos\theta\,a^2−2sinθcosθa2

at θ\thetaθ, in the sense of HasDerivAt.

Atom lemma of Layer II: the θ\thetaθ-derivative of Σ\SigmaΣ along the angular coordinate, consumed by hdgKerr_all and hdchrKerr_all through the chain rule.

Preamble
import Definitions.Def_KerrBL_Kerr_Metric
open KerrBL Filter Topology
Formal statement
theorem KerrBL.hasDerivAt_Sig_th (a r θ : ℝ) : HasDerivAt (fun θ => Sig a r (Real.cos θ)) (((-2))*Real.sin θ*Real.cos θ*a^(2:ℕ)) θ := by sorry
Source
R. P. Kerr, Gravitational field of a spinning mass as an example of algebraically special metrics, Phys. Rev. Lett. 11 (1963) 237-238, https://doi.org/10.1103/PhysRevLett.11.237; R. H. Boyer and R. W. Lindquist, Maximal analytic extension of the Kerr metric, J. Math. Phys. 8 (1967) 265-281, https://doi.org/10.1063/1.1705193, Sec. 2 (Boyer-Lindquist form of the Kerr line element); metric components transcribed token-for-token from the project certificate EinsteinSolver/certificate/kerr/metric.json (sha256 d729883d95fd7d3cf84d9c971c6725f847155562cc4e88660535b8d0bd0be336); design record LEAN/kerr-formalization/mission/DESIGN.md, node N3 (hasDerivAt_Sig_th)
Human review
  • Endorsed by Shuze Chen · Sep 14, 2026

  • Endorsed by He Wang · Sep 14, 2026

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

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