Case I, (14.23): source-faithful remainder interface #
The paper does not replace the two Lemma-8.7 endpoints by an arbitrary fixed
quotient. Claim 14.6(ii) licenses Lemma 8.7, Claim 14.6(iii) supplies the main
contraction, and the two remaining endpoint terms retain the literal coefficient
3 * (κ + 1) * K^2, hence 6 * K^2 in the production specialization κ = 1.
The paper's subsequent estimates contain σ^3 log (e σ). Consequently the
already accepted σ^2 scalar decay is necessary normalization data but is not,
by itself, the source estimate. The predicates below freeze the exact additional
source inequalities without choosing numerical constants hidden by the paper's
O notation.
Exact normalized unit used by every side remainder in (14.23).
Instances For
The literal Σ₁₁ Lemma-8.7 endpoint at τ=s, κ=1, β=2.
Equations
- MathlibNt.SieveTheory.caseI1423Sigma11Endpoint S N D z K s σ = MathlibNt.SieveTheory.SwitchingPrinciple.suzukiVProduct S ↑z * (6 * K ^ 2 * MathlibNt.SieveTheory.SuzukiFiniteContinuousLayers.finiteSourceLayer 1 2 (N - 1) (s - 1) / Real.log (↑D ^ (1 / σ)))
Instances For
The literal Σ₁₂ Lemma-8.7 endpoint at τ=s, κ=1.
This is definitionally the existing endpoint after cancelling s/s.
Equations
- MathlibNt.SieveTheory.caseI1423Sigma12Endpoint S H N D z C K d Δ s σ = C * Real.exp √K * MathlibNt.SieveTheory.SwitchingPrinciple.suzukiVProduct S ↑z * Real.log ↑D ^ (-Δ) * (6 * K ^ 2 * MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.qD H (MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign.ofDepth N).opposite (↑D) d Δ s / Real.log (↑D ^ (1 / σ)))
Instances For
Exact source scalar left in the Σ₁₁ endpoint calculation on p.87.
The existential coefficient is the honest interpretation of ≪; it is fixed
before D and works eventually.
Equations
- MathlibNt.SieveTheory.CaseI1423Sigma11SourceScalar K d Δ = ∃ (A : ℝ), 0 ≤ A ∧ ∀ᶠ (D : ℝ) in Filter.atTop, K ^ 2 * MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d ^ 3 * Real.log (Real.exp 1 * MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d) * Real.log (Real.log D) / Real.log D ^ (1 - Δ) ≤ A
Instances For
Exact source scalar left in the Σ₁₂ endpoint calculation on p.93.
It is deliberately not weakened to a fixed signed-layer quotient.
Equations
- MathlibNt.SieveTheory.CaseI1423Sigma12SourceScalar K d Δ = ∃ (A : ℝ), 0 ≤ A ∧ ∀ᶠ (D : ℝ) in Filter.atTop, K ^ 2 * MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d ^ 3 * Real.log (Real.exp 1 * MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d) * Real.log (Real.log D) / Real.log D ^ (1 - Δ) ≤ A
Instances For
Uniform Claim-14.6 source contract actually consumed before (14.19). One threshold is chosen before the sign and the moving coordinate. Part (ii) is the monotonicity input to Lemma 8.7; part (iii) is the strict integral bound which creates the main multiplier in (14.23).
Equations
- MathlibNt.SieveTheory.CaseI1423Claim146iiiiiSource H d Δ = ∃ (D₀ : ℝ), ∀ (D : ℝ), D₀ ≤ D → have σ := MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d; (∀ (sign : MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign), AntitoneOn (fun (t : ℝ) => MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.qD H sign.opposite D d Δ t * t) (Set.Ioc (2 + sign.epsilon) σ)) ∧ ∀ (sign : MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign) (s : ℝ), 2 + sign.epsilon ≤ s → s ≤ σ → ∫ (t : ℝ) in s..σ, MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.qD H sign.opposite D d Δ t < (1 - 1 / σ) ^ (1 - Δ) * MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.lambda H sign D d 0 s
Instances For
A numerical O-coefficient package for the two endpoint estimates.
The constants are selected before D; this is the uniformity needed in (14.23).
The hypotheses are the exact inequalities obtained after applying Claim 14.6(ii)
to Lemma 8.7 and then estimating the displayed endpoints on pp.87 and 93.
Equations
- MathlibNt.SieveTheory.CaseI1423EndpointSourceBounds = ∀ (S : BoundingSieve) (H : MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.Section13HatLayers) (N : ℕ) (C K d Δ s : ℝ), ∃ (A11 : ℝ) (A12 : ℝ), 0 ≤ A11 ∧ 0 ≤ A12 ∧ ∀ᶠ (D : ℕ) in Filter.atTop, have σ := MathlibNt.SieveTheory.SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma (↑D) d; have z := ⌈↑D ^ (1 / s)⌉₊; have B := MathlibNt.SieveTheory.sigma12InheritedBudget S H N D z C K d Δ s; MathlibNt.SieveTheory.caseI1423Sigma11Endpoint S N D z K s σ ≤ A11 * MathlibNt.SieveTheory.caseI1423RemainderUnit B (↑D) σ ∧ MathlibNt.SieveTheory.caseI1423Sigma12Endpoint S H N D z C K d Δ s σ ≤ A12 * MathlibNt.SieveTheory.caseI1423RemainderUnit B (↑D) σ
Instances For
Exact finite algebra behind the endpoint part of (14.23): the two source
remainders combine with coefficient A11 + A12, with no generic quotient and
no absorption premise.
Eventual endpoint combination with all source quantifiers in their required
order. In particular A11,A12 are independent of D.