System (4) system (7), equation
ProvedHintz2026.system7_zminus_of_system4differential-geometryexact-vacuum-atlas-iiigeneral-relativitymathematical-physics
Let be fields on and . Suppose the second equation of Hintz's chiral system (4) holds at :
Then and satisfy at
The proof uses the Leibniz rule for , to cancel the -term, and the closed form together with .
Preamble
import Definitions.Def_Hintz2026_System4 open Hintz2026 Complex Matrix Function open scoped ComplexConjugate ContDiff
Formal statement
theorem Hintz2026.system7_zminus_of_system4 (p : SubextremalKN) (yplus yminus : (Fin 2 -> ℝ) -> Fin 2 -> ℂ) (sg om mm : ℝ) (hyp : ∀ j : Fin 2, ContDiffOn ℝ ∞ (fun x => yplus x j) (U p)) (hym : ∀ j : Fin 2, ContDiffOn ℝ ∞ (fun x => yminus x j) (U p)) {x : Fin 2 -> ℝ} (hx : x ∈ U p) (h4 : (fun j => Dp p (fun z => yminus z j) x) + A p x *ᵥ yminus x = (cscalar p sg om mm x • (1 : Matrix (Fin 2) (Fin 2) ℂ) + Bmat p sg om mm x) *ᵥ yplus x) : (fun i => Dp p (fun z => ((X p z)ᴴ *ᵥ yminus z) i) x) = adjugate (Cmat p sg om mm x) *ᵥ zplus p yplus x := by sorrySource
Hintz, Perturbations of Kerr-Newman black holes: separation and mode stability, arXiv:2609.33661v1, Section 2 eq. (7)/(8) and the text after (7); local source Atlas/Perturbations/Hintz2026/Equivalence4to7.lean at commit 8d059e0 (no public Git remote)
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.