B-suffixed KN spin coefficients
ProvedExactVacuumAtlas.EinsteinMaxwell.NP.npKN_Beinstein-maxwellexact-spacetime-atlas-vexact-vacuum-atlasgeneral-relativitynewman-penrose
B-suffixed KN spin coefficients
On domReg, the theorem gives the eight displayed KN background formulas for npRhoB, npTauB, npPiB, npMuB, npEpsB, npBetaB, npAlphaB and npGammaB. These are the B-suffixed, index-swapped spin coefficients; npKappaB is not one of the conclusions of this node. The theorem does not assert a numerical conjugation rule for complexified variations.
Scope. Exactly the hypotheses printed in the formal statement.
中文摘要 KN 背景的八个 B 后缀系数闭式:RhoB、TauB、PiB、MuB、EpsB、BetaB、AlphaB、GammaB;本条不包含 KappaB,也不对复化扰动附加数值共轭规则。
Preamble
import Mathlib
import Definitions.Def_Atlas_Core_Basic
import Definitions.Def_Atlas_Core_Lift
import Definitions.Def_Atlas_EinsteinMaxwell_Basic
import Definitions.Def_Atlas_EinsteinMaxwell_Certificate
import Definitions.Def_Atlas_EinsteinMaxwell_KN_Defs
import Definitions.Def_Atlas_EinsteinMaxwell_KN_Domain
import Definitions.Def_Atlas_EinsteinMaxwell_NP_Basic
import Definitions.Def_Atlas_EinsteinMaxwell_NP_Bianchi
import Definitions.Def_Atlas_EinsteinMaxwell_NP_CCalc
import Definitions.Def_Atlas_EinsteinMaxwell_NP_FrameConn
import Definitions.Def_Atlas_EinsteinMaxwell_NP_FrameNull
import Definitions.Def_Atlas_EinsteinMaxwell_NP_KNComm
import Definitions.Def_Atlas_EinsteinMaxwell_NP_KNFaraday
import Definitions.Def_Atlas_EinsteinMaxwell_NP_KNFrame
import Definitions.Def_Atlas_EinsteinMaxwell_NP_KNSpin
import Definitions.Def_Atlas_EinsteinMaxwell_NP_KNWeyl
import Definitions.Def_Atlas_EinsteinMaxwell_NP_ModeOperators
import Definitions.Def_Atlas_EinsteinMaxwell_NP_NPBianchi
import Definitions.Def_Atlas_EinsteinMaxwell_NP_NPMaxwell
import Definitions.Def_Atlas_EinsteinMaxwell_NP_NPRicci
import Definitions.Def_Atlas_EinsteinMaxwell_NP_NPScalars
import Definitions.Def_Atlas_EinsteinMaxwell_NP_Riemann
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03C3
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Cplx
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Family
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03LinKN
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03LinMx
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Mode
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Realize
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Res
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Src
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Tan
import Definitions.Def_Atlas_EinsteinMaxwell_NP_V03Var
import Definitions.Def_Atlas_EinsteinMaxwell_Variation_Defs
import Definitions.Def_Atlas_EinsteinMaxwell_Variation_Local
import Definitions.Def_Atlas_Kerr_InAtoms
import Definitions.Def_Atlas_Transport_Connection
import Definitions.Def_Atlas_Transport_MatrixCalc
import Definitions.Def_Hintz2026_Chiral
import Definitions.Def_Hintz2026_Core
import Definitions.Def_Hintz2026_Domain
import Definitions.Def_Hintz2026_System1
import Definitions.Def_Hintz2026_System4
open Complex Filter Topology
open scoped ComplexConjugate Matrix ContDiff
open ExactVacuumAtlas.EinsteinMaxwell ExactVacuumAtlas.Variation
open ExactVacuumAtlas.EinsteinMaxwell.KN (Sig Del gKN giKN domReg domKN faradayKN)
open ExactVacuumAtlas
open ExactVacuumAtlas.EinsteinMaxwell
open ExactVacuumAtlas.EinsteinMaxwell.NP
variable {M a Q : ℝ} {x : Pt 4}
Formal statement
theorem ExactVacuumAtlas.EinsteinMaxwell.NP.npKN_B (hx : x ∈ domReg M a Q) :
npRhoB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x = -1 / qK a x ∧
npTauB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x
= I * ((a * Real.sin (x 2) : ℝ) : ℂ) / (((Real.sqrt 2 : ℝ) : ℂ) * ((Sig a (x 1) (x 2) : ℝ) : ℂ)) ∧
npPiB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x
= -(I * ((a * Real.sin (x 2) : ℝ) : ℂ)) / (((Real.sqrt 2 : ℝ) : ℂ) * qK a x ^ 2) ∧
npMuB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x
= -((Del M a Q (x 1) : ℝ) : ℂ) / (2 * ((Sig a (x 1) (x 2) : ℝ) : ℂ) * qK a x) ∧
npEpsB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x = 0 ∧
npBetaB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x
= ((Real.cos (x 2) / Real.sin (x 2) : ℝ) : ℂ) / (2 * ((Real.sqrt 2 : ℝ) : ℂ) * qbarK a x) ∧
npAlphaB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x
= -(I * ((a * Real.sin (x 2) : ℝ) : ℂ)) / (((Real.sqrt 2 : ℝ) : ℂ) * qK a x ^ 2)
- ((Real.cos (x 2) / Real.sin (x 2) : ℝ) : ℂ) / (2 * ((Real.sqrt 2 : ℝ) : ℂ) * qK a x) ∧
npGammaB (gKN M a Q) (giKN M a Q) (knE M a Q) (knTh M a Q) x
= -((Del M a Q (x 1) : ℝ) : ℂ) / (2 * ((Sig a (x 1) (x 2) : ℝ) : ℂ) * qK a x)
+ (((x 1 - M) / (2 * Sig a (x 1) (x 2)) : ℝ) : ℂ) := by sorrySource
He Wang, Exact Spacetime Atlas V: From Linearized Einstein–Maxwell Equations to Kerr–Newman Radiation Systems. Local source, no public repository; commit b8cd107a558e153ed41fb4972ac5315499d14778; Atlas/EinsteinMaxwell/NP/V03Res.lean#L26-L48; SHA-256 428706d4df792e38c8711c2b24c8ab30316521cacd37941872e4003eb33e73a5. Registered definitions: mission/PHYSICS_BOUNDARY.md (§K–§M); literature: P. Hintz, arXiv:2609.33661 (v1); Mark–Yang–Zimmerman–Chen, arXiv:1409.5800 (v1).
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.