OAI/NumberTheory/Ostmann/Arithmetic/RestoredHarmonicCells.lean
3 declarations, 0 contain sorry, 0 declared as axioms
Restoring exceptional prime atoms with the original normalization
- theorem
OAI.Ostmann.primeSubsetLogMeasure_restored_massline 11 - theorem
OAI.Ostmann.PublishedProgressionInput.harmonic_cells_mass_errorline 21Source documentation
The modulus-one comparison gives the exact error in replacing all harmonic prime atoms by the real harmonic masses of the cells.
theorem PublishedProgressionInput.harmonic_cells_mass_error (P : PublishedProgressionInput) {C : Type*} [Fintype C] (Q : ℕ) (hQ : 2 ≤ Q) (u v : C → ℝ) (hu : ∀ c, 1 ≤ u c) (huv : ∀ c, u c ≤ v c) (hshort : ∀ c, v c ≤ u c + 1) (Z : ℝ) (hZ : 0 ≤ Z) : |(bulkCellMixture Z (fun c => primeLogCellMeasure 1 0 (u c) (v c))).real Set.univ - Z * ∑ c, ∫ x in Set.Ioc (u c) (v c), (x : ℝ)⁻¹| ≤ Z * ∑ c, bulkPrimeErrorFactor P Q (u c) := by …Mentions: OAI.Ostmann.PublishedProgressionInput, OAI.Ostmann.bulkCellMixture, OAI.Ostmann.primeLogCellMeasure, OAI.Ostmann.bulkPrimeErrorFactor
- theorem
OAI.Ostmann.PublishedProgressionInput.restored_harmonic_cells_le_twoline 46Source documentation
Small exceptional deletions and the interval error share the same unit error budget, while the normalization remains that of the deleted prime set.
theorem PublishedProgressionInput.restored_harmonic_cells_le_two (P : PublishedProgressionInput) {C : Type*} [Fintype C] (Q : ℕ) (hQ : 2 ≤ Q) (u v : C → ℝ) (hu : ∀ c, 1 ≤ u c) (huv : ∀ c, u c ≤ v c) (hshort : ∀ c, v c ≤ u c + 1) (hsep : ∀ c d, c ≠ d → v c ≤ u d ∨ v d ≤ u c) (D : Finset ℕ) (hS : (∑ p ∈ primeCellSupport 1 (fun _ => 0) u v \ D, (p : ℝ)⁻¹) ≠ 0) (herror : (∑ p ∈ primeCellSupport 1 (fun _ => 0) u v \ D, (p : ℝ)⁻¹)⁻¹ * ((∑ p ∈ primeCellSupport 1 (fun _ => 0) u v ∩ D, (p : ℝ)⁻¹) + ∑ c, bulkPrimeErrorFactor P Q (u c)) ≤ 1) : (∑ p ∈ primeCellSupport 1 (fun _ => 0) u v \ D, (p : ℝ)⁻¹)⁻¹ * …Mentions: OAI.Ostmann.PublishedProgressionInput, OAI.Ostmann.primeCellSupport, OAI.Ostmann.bulkPrimeErrorFactor