OAI/Geometry/EinsteinFour/ScalarPoissonKernelLocalizationChain.lean
3 declarations, 0 contain sorry, 0 declared as axioms
A finite chain of nested cutoffs upgrades local H1 control to every requested finite Sobolev order. Only the localized equation's right-hand side needs that order; the starting solution needs one derivative.
- theorem
OAI.PositiveEinsteinFour.Geometry.scalar_finite_cutoff_chain_gainline 25Source documentation
nnested transitions upgrade an outer H1 cutoff to H^(n+1) at the innermost cutoff. The sequence outside the finite chain is irrelevant.theorem scalar_finite_cutoff_chain_gain (a : Fin 4 → Fin 4 → S) (b : Fin 4 → S) (δ : ℝ) (hδ : 0 ≤ δ) (ha : ∀ i j x, ‖a i j x‖ ≤ δ) (ha1 : ∀ i j k x, ‖D k (a i j) x‖ ≤ δ) (ha2 : ∀ i j k l x, ‖D k (D l (a i j)) x‖ ≤ δ) (hb : ∀ i x, ‖b i x‖ ≤ δ) (hb1 : ∀ i k x, ‖D k (b i) x‖ ≤ δ) (hsmall : (16 * (2 * Real.pi) ^ 2 + 36 * (2 * Real.pi) + 20) * δ < 1) (u : T) (n : ℕ) (ψ : ℕ → S) (hnest : ∀ k < n, ScalarCutoffNested (ψ k) (ψ (k + 1))) (hu : MemSobolev 1 2 (M (ψ n) u)) (hf : ∀ k ≤ n, MemSobolev (n : ℝ) 2 (M (ψ k) (scalarPerturbedOperator a b u))) : …Mentions: OAI.PositiveEinsteinFour.Geometry.ScalarCutoffNested, OAI.PositiveEinsteinFour.Geometry.scalarPerturbedOperator
- theorem
OAI.PositiveEinsteinFour.Geometry.scalar_cutoff_family_all_ordersline 58Source documentation
A family of finite localizing chains gives all integer Sobolev orders for a fixed inner cutoff. This is the form used before Fourier inversion.
theorem scalar_cutoff_family_all_orders (a : Fin 4 → Fin 4 → S) (b : Fin 4 → S) (δ : ℝ) (hδ : 0 ≤ δ) (ha : ∀ i j x, ‖a i j x‖ ≤ δ) (ha1 : ∀ i j k x, ‖D k (a i j) x‖ ≤ δ) (ha2 : ∀ i j k l x, ‖D k (D l (a i j)) x‖ ≤ δ) (hb : ∀ i x, ‖b i x‖ ≤ δ) (hb1 : ∀ i k x, ‖D k (b i) x‖ ≤ δ) (hsmall : (16 * (2 * Real.pi) ^ 2 + 36 * (2 * Real.pi) + 20) * δ < 1) (u : T) (φ : S) (hchain : ∀ n : ℕ, ∃ ψ : ℕ → S, ψ 0 = φ ∧ (∀ k < n, ScalarCutoffNested (ψ k) (ψ (k + 1))) ∧ MemSobolev 1 2 (M (ψ n) u) ∧ …Mentions: OAI.PositiveEinsteinFour.Geometry.ScalarCutoffNested
- theorem
OAI.PositiveEinsteinFour.Geometry.scalar_cutoff_family_smooth_representativeline 81Source documentation
The regular representative is constructed by the Fourier Sobolev theorem, once the finite cutoff chains have been supplied.
theorem scalar_cutoff_family_smooth_representative (a : Fin 4 → Fin 4 → S) (b : Fin 4 → S) (δ : ℝ) (hδ : 0 ≤ δ) (ha : ∀ i j x, ‖a i j x‖ ≤ δ) (ha1 : ∀ i j k x, ‖D k (a i j) x‖ ≤ δ) (ha2 : ∀ i j k l x, ‖D k (D l (a i j)) x‖ ≤ δ) (hb : ∀ i x, ‖b i x‖ ≤ δ) (hb1 : ∀ i k x, ‖D k (b i) x‖ ≤ δ) (hsmall : (16 * (2 * Real.pi) ^ 2 + 36 * (2 * Real.pi) + 20) * δ < 1) (u : T) (φ : S) (hchain : ∀ n : ℕ, ∃ ψ : ℕ → S, ψ 0 = φ ∧ (∀ k < n, ScalarCutoffNested (ψ k) (ψ (k + 1))) ∧ MemSobolev 1 2 (M (ψ n) u) ∧ …Mentions: OAI.PositiveEinsteinFour.Geometry.ScalarCutoffNested