Atlas VII definitions: VII16AsymptoticBridge
DefinitionAtlas_EinsteinMaxwell_ES5_KerrSchild_VII16AsymptoticBridgeDefinitions of the Atlas VII module Atlas.EinsteinMaxwell.ES5.KerrSchild.VII16AsymptoticBridge (kept exactly as in the accepted source, skeleton subtraction).
VII16 — the finite asymptotic bridge (sufficiency direction)
Real germs on (0, ε) whose iterated derivatives 0 … n have finite right limits at the
origin. Glue the negative side to the Taylor polynomial of those limits. The result is a
genuine Cⁿ function on (-ε, ε) agreeing with the germ on the positive side — exactly the
regularity interface FiniteBranch6 needs.
The derivative limits are an INPUT. notes/VII16_ASYMPTOTIC_ANALYSIS.md records that the
paper's §3.1 supplies value-level asymptotics (Eq. 30/33) and a chosen formal integer-power
series (Eq. 32/36), not derivative asymptotics. The converse (paper branch ⇒ these limits) is
not established in this round, so the original goal stays conditional.
Constants in this bundle: flatExt, glue, taylorPoly.
Registered B3 definition layer (Mathlib at the pinned revision has no Lorentzian metric / Ricci API): mission/PHYSICS_BOUNDARY.md, Atlas VII sections P–XVII.
-- Generated by scripts/vii24r/publish/gen_platform_tree_unitA.py (Atlas VII Unit A; copy of the RELEASE06 generator, header only) by skeleton subtraction from Atlas/EinsteinMaxwell/ES5/KerrSchild/VII16AsymptoticBridge.lean -- definition bundle: kept ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16.flatExt, ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16.glue, ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16.taylorPoly import Mathlib import Definitions.Def_Atlas_Core_Basic import Definitions.Def_Atlas_EinsteinMaxwell_Basic import Definitions.Def_Atlas_EinsteinMaxwell_D_Basic import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Defs import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Cert import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Data import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Reduced import Definitions.Def_Atlas_EinsteinMaxwell_ES5_Generic_Tables import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_CompactifiedBridge import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_CompactifiedResiduals import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_FiniteJetObstruction import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_FiniteTaylorJet import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_JetRecursion import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_OneSidedExtraction import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_PaperGauge import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_PolynomialJet import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_RadialBVP import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_RadialBVPEquivalence import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_ScalarCertificate import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_SmoothBranch import Definitions.Def_Atlas_EinsteinMaxwell_ES5_KerrSchild_VII13FiniteBranchSpec /-! # VII16 — the finite asymptotic bridge (sufficiency direction) Real germs on `(0, ε)` whose iterated derivatives `0 … n` have finite right limits at the origin. Glue the negative side to the Taylor polynomial of those limits. The result is a genuine `Cⁿ` function on `(-ε, ε)` agreeing with the germ on the positive side — exactly the regularity interface `FiniteBranch6` needs. **The derivative limits are an INPUT.** `notes/VII16_ASYMPTOTIC_ANALYSIS.md` records that the paper's §3.1 supplies value-level asymptotics (Eq. 30/33) and a *chosen* formal integer-power series (Eq. 32/36), not derivative asymptotics. The converse (paper branch ⇒ these limits) is not established in this round, so the original goal stays conditional. -/ open Filter Set open scoped Topology ContDiff open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.Compact (pull pullM) open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII13FiniteBranchSpec (FiniteBranch6) -- (open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.SmoothExt.Controls: no listed name exists here) -- (open ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.Radial: no listed name exists here) namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## Negative-side Taylor polynomial -/ /-- Negative-side Taylor polynomial with prescribed jet `L`. -/ noncomputable def taylorPoly (L : ℕ → ℝ) (n : ℕ) : ℝ → ℝ := fun x => ∑ k ∈ Finset.range (n + 1), L k / (k.factorial : ℝ) * x ^ k /-! ## The flat extension -/ /-- Extend a function on `(0, ε)` by zero to the left of the origin. -/ noncomputable def flatExt (h : ℝ → ℝ) : ℝ → ℝ := fun x => if 0 < x then h x else 0 /-! ## Continuity -/ /-! ## Derivative at the origin and the derivative identity -/ end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## The Cⁿ induction -/ end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## The glued germ: polynomial on the left, the actual germ on the right -/ /-- Glue: Taylor polynomial below `0`, the actual germ above. Written as polynomial plus a flat correction so that the flat-extension theory applies unchanged. -/ noncomputable def glue (L : ℕ → ℝ) (n : ℕ) (g : ℝ → ℝ) : ℝ → ℝ := fun x => taylorPoly L n x + flatExt (fun y => g y - taylorPoly L n y) x end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## From derivative limits to the `C⁶` gluing -/ end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## One-sided C⁶ germs of the actual pull-backs -/ /-! ## The main assembly -/ end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## Negative control: value asymptotics do not give derivative control `x ↦ 1 + x⁷ sin((x⁸)⁻¹)` on `(0, ∞)` has value remainder `O(x⁷)`: **every** value coefficient below order 7 is that of the constant `1`. Its actual derivative, however, is `7x⁶ sin(x⁻⁸) − 8x⁻² cos(x⁻⁸)` (the outer `x⁷` cancels one power of `x` in `x¹⁴/x¹⁶`), whose second term grows like `x⁻²` and oscillates in sign, so the derivative has no finite right limit at `0⁺`. The no-limit conclusion itself is an analysis argument (`notes/VII16_ASYMPTOTIC_ANALYSIS.md` §6); only the two algebraic facts above are formalised in Lean. This function is **not** an Einstein–Maxwell solution. It refutes only the inference "value expansion ⇒ differentiable control", which is precisely the inference the paper's Eq. (30)/(33) do not license and which `FiniteBranch6` requires. -/ end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 /-! ## Positive control: the real RN branch through the new bridge Reissner–Nordström with `Q = 3/4`, `J = 0`. The extension `rnExtF`, `rnExtb` is a *ratio of polynomials*, so its iterated derivatives at the origin exist and are given by the rational function itself; the derivative limits required by `finiteBranch6_of_deriv_limits` are therefore discharged **from the actual pull-backs**, not assumed as a `FiniteBranch6` premise. -/ end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 namespace ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16 end ExactVacuumAtlas.EinsteinMaxwell.ES5.KerrSchild.VII16