Low-band continuum mass is negligible on the cubic logarithmic scale
ProvedErdos390.Full.RegularMeshPrimeCutoffs.Mesh.tendsto_low_endpointContinuumMass_div_log_y_cube_zeroanalytic-number-theoryerdos-390erdos390-source-construction
Write , , , and . Let be a regular relative mesh with and let . For its low band, let be the consecutive full endpoint cutoffs and put . Then
This controls the growth of the low continuum harmonic mass in estimates involving a reciprocal moving center.
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_002 import Definitions.Def_erdos390_analytic_foundations_003 import Definitions.Def_erdos390_analytic_foundations_005
Formal statement
theorem Erdos390.Full.RegularMeshPrimeCutoffs.Mesh.tendsto_low_endpointContinuumMass_div_log_y_cube_zero :
∀ {delta eta : Real} (M : Erdos390.Full.RegularRelativeMesh.Mesh delta eta),
LT.lt.{0} (0 : Real) delta →
∀ {W : Nat},
LE.le.{0} (2 : Nat) W →
Filter.Tendsto.{0, 0}
(fun n =>
HDiv.hDiv.{0, 0, 0}
(Erdos390.Full.RegularMeshPrimeCutoffs.Mesh.endpointContinuumMass M n W
(Erdos390.Full.RegularMeshPrimeCutoffs.Mesh.lowBand M))
(HPow.hPow.{0, 0, 0} (Real.log (Erdos390.Full.ArithmeticModel.y n)) (3 : Nat)))
Filter.atTop.{0} (nhds.{0} (0 : Real)) := by sorry
Source