theorem
MathlibNt.SieveTheory.caseIIPositiveDeltaIntegralPart_source_exact_relative
(H : SwitchingPrinciple.SuzukiLemma144KappaOne.Section13HatLayers)
{N : ℕ}
{D d Δ σ C K s : ℝ}
(hD : 1 < D)
(hs : 0 < s)
(hC : 0 ≤ C)
(hK : 0 ≤ K)
(hcut : 0 ≤ (1 - 1 / σ) ^ (1 - Δ))
(hiii :
∫ (t : ℝ) in 3..σ, SwitchingPrinciple.SuzukiLemma144KappaOne.qD H
(SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign.ofDepth N).opposite D d Δ t ≤ (1 - 1 / σ) ^ (1 - Δ) * SwitchingPrinciple.SuzukiLemma144KappaOne.lambda H (SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign.ofDepth N)
D d 0 3)
(hcubic :
SwitchingPrinciple.SuzukiLemma144KappaOne.lambda H (SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign.ofDepth N) D d
0 3 ≤ SwitchingPrinciple.SuzukiLemma144KappaOne.perturbation D d 0 3 * SwitchingPrinciple.SuzukiLemma144KappaOne.lambda H (SwitchingPrinciple.SuzukiLemma144KappaOne.ErrorSign.ofDepth N)
D d 0 s)
:
At the exact source point y = D^(1/3), the integral contribution pays
both the cubic lambda comparison and the product-ratio excess.
theorem
MathlibNt.SieveTheory.exists_integral_transport_relative_excess_threshold
(Δ d K : ℝ)
(hΔ0 : 0 < Δ)
(hΔ1 : Δ < 1)
(hd : 7 / (1 - Δ) < d)
(hK : 0 ≤ K)
:
∃ (D0 : ℝ),
1 < D0 ∧ ∀ (D : ℝ),
D0 ≤ D →
(1 + 3 * K / Real.log D) * (1 - 1 / SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d) ^ (1 - Δ) * SwitchingPrinciple.SuzukiLemma144KappaOne.perturbation D d 0 3 - (1 - 1 / SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d) ^ (1 - Δ) ≤ (1 - Δ) / (32 * SwitchingPrinciple.SuzukiLemma144KappaOne.sourceSigma D d)
Eventually the transported relative integral coefficient pays both the cubic perturbation and the local product-ratio excess.