OAI/NumberTheory/JointDickman/Counting/SignedCoefficientSums.lean
7 declarations, 0 contain sorry, 0 declared as axioms
Exact sign reversal for the coefficient relation a - b = jc
- def
OAI.JointDickman.coefficientRelationWeightline 14 - def
OAI.JointDickman.signedCoefficientMassline 18 - theorem
OAI.JointDickman.coefficientRelationWeight_negline 21 - theorem
OAI.JointDickman.signedCoefficientMass_negline 28 - theorem
OAI.JointDickman.coefficientRelationWeight_natline 34 - theorem
OAI.JointDickman.signedCoefficientMass_nat_leline 47 - theorem
OAI.JointDickman.signed_coefficient_three_form_boundline 66Source documentation
Both signs of the lag satisfy the same rectangle bound, including the support restriction that both a and b belong to the coefficient interval.
theorem signed_coefficient_three_form_bound (hFord : PublishedInputs.FordUpperSieveInput) (hM : PublishedInputs.PrimeReciprocalMertensInput) {δ : ℝ} (hδ : 0 < δ) : ∃ C : ℝ, 0 < C ∧ ∀ᶠ B : ℕ in atTop, ∀ (j : ℤ) (u v w x : ℕ), j ≠ 0 → u ≤ v → w ≤ x → Real.exp (δ * B) ≤ (v : ℝ) - u → Real.exp (δ * B) ≤ (x : ℝ) - w → signedCoefficientMass B j (Ico u v) (Ico w x) ≤ C * ((v : ℝ) - u) * ((x : ℝ) - w) * singularFactor 24 j.natAbs := by …Mentions: OAI.JointDickman.PublishedInputs.FordUpperSieveInput, OAI.JointDickman.PublishedInputs.PrimeReciprocalMertensInput, OAI.JointDickman.signedCoefficientMass, OAI.JointDickman.singularFactor