The chamber remainder preserves two logarithmic decay rates
ProvedErdos390.Full.PaperPrimePowerRemainderRate.tendsto_primePowerChamberRemainder_mul_logL_sq_zeroanalytic-number-theoryerdos-390erdos390-source-construction
Write , for the fixed Dickman constant, , , and . Thus is the source's common prime-power chamber remainder. For arbitrary real , natural , and real sequence , assume and . Then
This supplies the additional decay needed before summing over a harmonic prime row.
Preamble
import Mathlib import Definitions.Def_erdos390_source_bank_interface import Definitions.Def_erdos390_dickman_step_function import Theorems.Thm_MediumPNT import Definitions.Def_erdos390_analytic_foundations_001 import Theorems.Thm_Erdos390_Full_DickmanBasic_kernel_product_bound import Theorems.Thm_Erdos390_Full_DickmanBasic_rho_pos_on_zero_five import Theorems.Thm_Erdos390_Full_DickmanBasic_kernel_secondDerivative_first_bound import Definitions.Def_erdos390_analytic_foundations_004
Formal statement
theorem Erdos390.Full.PaperPrimePowerRemainderRate.tendsto_primePowerChamberRemainder_mul_logL_sq_zero :
∀ (epsilon : Nat → Real) (G₀ B : Real) (W : Nat),
Filter.Tendsto.{0, 0} epsilon Filter.atTop.{0} (nhds.{0} (0 : Real)) →
Filter.Tendsto.{0, 0}
(fun n => HMul.hMul.{0, 0, 0} (epsilon n) (HPow.hPow.{0, 0, 0} (Real.log (Erdos390.Full.Scale.L n)) (2 : Nat)))
Filter.atTop.{0} (nhds.{0} (0 : Real)) →
Filter.Tendsto.{0, 0}
(fun n =>
HMul.hMul.{0, 0, 0}
(Erdos390.Full.PaperPrimePowerFourDisplays.primePowerChamberRemainder (epsilon n) G₀
(Erdos390.Full.PaperPrimePowerChamberError.coefficientScale B W n))
(HPow.hPow.{0, 0, 0} (Real.log (Erdos390.Full.Scale.L n)) (2 : Nat)))
Filter.atTop.{0} (nhds.{0} (0 : Real)) := by sorry
Source