OAI/NumberTheory/TotientAsymptotic/VolumeComparison.lean
9 declarations, 0 contain sorry, 0 declared as axioms
The banded perturbed volume and the exact finite coefficient differ by a vanishing normalized error.
- def
OAI.TotientAsymptotic.exactWitnessUnionline 15 - def
OAI.TotientAsymptotic.perturbedWitnessUnionline 18 - lemma
OAI.TotientAsymptotic.bandedWitnessRegion_eqline 22 - lemma
OAI.TotientAsymptotic.exactWitnessUnion_volume_ne_topline 33 - lemma
OAI.TotientAsymptotic.perturbedWitnessUnion_volume_ne_topline 38 - lemma
OAI.TotientAsymptotic.exactWitnessUnion_empty_of_not_totientline 47 - lemma
OAI.TotientAsymptotic.unionVolumeCoefficient_mul_Gline 57 - lemma
OAI.TotientAsymptotic.perturbed_exact_volume_differenceline 72 - theorem
OAI.TotientAsymptotic.banded_volume_coefficient_approximationline 99Source documentation
The geometric approximation to the exact coefficient. Only the prime-grid-to-volume step remains in the mass approximation after this.
theorem banded_volume_coefficient_approximation (hbox : FordUnitPrimeBoxInput) (hmertens : MertensProductInput) (hren : FordRenewalInput) (hford : FordCoordinateConcentrationInput) : ∃ ε : ℕ → ℝ, Tendsto ε atTop (nhds 0) ∧ ∀ᶠ H : ℕ in atTop, ∀ᶠ x : ℝ in atTop, ∀ f : ℝ → ℝ, (∀ r, 0 ≤ f r ∧ f r ≤ 1) → |bandedVolumeMass x H f/G x (m x)-unionVolumeCoefficient H f x| ≤ ε H := by …Mentions: OAI.TotientAsymptotic.FordUnitPrimeBoxInput, OAI.TotientAsymptotic.MertensProductInput, OAI.TotientAsymptotic.FordRenewalInput, OAI.TotientAsymptotic.FordCoordinateConcentrationInput, OAI.TotientAsymptotic.bandedVolumeMass, OAI.TotientAsymptotic.G, OAI.TotientAsymptotic.m, OAI.TotientAsymptotic.unionVolumeCoefficient