The RN b-direction has vanishing Maxwell and Faraday linearised residuals
ProvedExactVacuumAtlas.Variation.RN.b_tangent_maxwell_closedeinstein-maxwellexact-spacetime-atlas-ivexact-vacuum-atlasgeneral-relativity
The RN b-direction has vanishing Maxwell and Faraday linearised residuals
For all real M, Q and x ∈ domRN: LJ^b(gRN M (Q²), giRN M (Q²), faradayRN Q; tanB, 0)(x) = 0 for all b and LH_abc(0)(x) = 0.
Scope. Same direction as nonzero_theta.
中文摘要 同一方向的 Maxwell 与闭合线性残差为零(只有 Einstein 部分非零)。
Preamble
import Mathlib import Definitions.Def_Atlas_Core_Basic import Definitions.Def_Atlas_Core_Certificate import Definitions.Def_Atlas_Core_Lift import Definitions.Def_Atlas_EinsteinMaxwell_Basic import Definitions.Def_Atlas_EinsteinMaxwell_Certificate import Definitions.Def_Atlas_EinsteinMaxwell_RN_Defs import Definitions.Def_Atlas_EinsteinMaxwell_RN_Frame import Definitions.Def_Atlas_EinsteinMaxwell_Variation_Defs import Definitions.Def_Atlas_EinsteinMaxwell_Variation_RN import Definitions.Def_Atlas_Transport_MatrixCalc open Real open scoped ContDiff open ExactVacuumAtlas.EinsteinMaxwell ExactVacuumAtlas.EinsteinMaxwell.RN
Formal statement
theorem ExactVacuumAtlas.Variation.RN.b_tangent_maxwell_closed (M Q : ℝ) {x : Pt 4} (hx : x ∈ domRN) :
(∀ b, linMaxwell (gRN M (Q ^ 2)) (giRN M (Q ^ 2)) (faradayRN Q) tanB 0 b x = 0) ∧
(∀ a b c, linFaraday (0 : TwoForm 4) a b c x = 0) := by sorrySource
He Wang, Exact Spacetime Atlas IV: Certified Einstein–Maxwell Backgrounds and First Variations. Local source, no public repository; commit 543904bfcfa3bb169f43fc4d9dbd569999b71886; Atlas/EinsteinMaxwell/Variation/RN.lean#L177-L187; SHA-256 7513cd6c91a5e550bb62e1cac2f2c8a8c17fa469087ba3c27bf9c1eab933f66f. Registered definitions and literature: mission/PHYSICS_BOUNDARY.md (§H–§J); Müller–Grave arXiv:0904.4184; Newman et al., J. Math. Phys. 6 (1965) 918.
Human review
Confirmed by the mission captain (proposal self-audit).
Confirmed by the moderator at approval.