OAI/NumberTheory/JointDickman/Probability/OrientedSplitBound.lean
4 declarations, 0 contain sorry, 0 declared as axioms
One oriented change interval in the actual conditional split law
- def
OAI.JointDickman.additionRatioTestline 13 - def
OAI.JointDickman.orientedSplitMassline 18 - theorem
OAI.JointDickman.additionRatioTest_averageline 29 - theorem
OAI.JointDickman.oriented_split_boundline 44Source documentation
The no-high-change probability and the low ratio probability multiply in the exact conditional law. This statement retains the actual high masses.
theorem oriented_split_bound (hFord : PublishedInputs.FordUpperSieveInput) (hM : PublishedInputs.PrimeReciprocalMertensInput) (κ : ℝ) : ∃ K : ℝ, 0 < K ∧ ∀ᶠ B : ℕ in atTop, ∀ (A D : Finset ℕ) (Y C T : ℝ), A ⊆ auxiliaryPrimes B → D ⊆ auxiliaryPrimes B → (∏ p ∈ A, p : ℕ) ≤ Real.exp (κ * B) → 0 < Y → Real.log (auxiliaryCutoff B) ≤ Y → Y ≤ 8 * B → 0 < T → orientedSplitMass B A D Y C T ≤ (1 / 2 : ℝ)^(A ∩ upperAdditionPrimes B Y).card * (1 / 2 : ℝ)^(D ∩ upperAdditionPrimes B Y).card * (highNoAdditionMass (upperAdditionPrimes B Y) (remainingPrimeParameter D) ((2 / 5 : ℝ) * Real.log ((B : ℝ) / Y) - C) * …Mentions: OAI.JointDickman.PublishedInputs.FordUpperSieveInput, OAI.JointDickman.PublishedInputs.PrimeReciprocalMertensInput, OAI.JointDickman.auxiliaryPrimes, OAI.JointDickman.auxiliaryCutoff, OAI.JointDickman.orientedSplitMass, OAI.JointDickman.upperAdditionPrimes, OAI.JointDickman.highNoAdditionMass, OAI.JointDickman.remainingPrimeParameter