A canonical logarithmic grid for Liu's prime pairs #
This module partitions the fixed source box
(1/10, 1/3] × (1/3, 9/20] into an n × n grid. Cells are selected from
their lower-left corners using the exact source boundary α + 2β ≤ 1.
The resulting finite rectangle majorant converges, for each fixed positive
n, to its logarithmic upper sum.
No limit as the mesh tends to zero is asserted here.
The ith point of the canonical alpha grid from 1/10 to 1/3.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n i = 1 / 10 + ↑i / ↑n * (7 / 30)
Instances For
The jth point of the canonical beta grid from 1/3 to 9/20.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n j = 1 / 3 + ↑j / ↑n * (7 / 60)
Instances For
The alpha width of a cell in the canonical grid.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuAlphaGridStep n = 7 / 30 / ↑n
Instances For
The beta width of a cell in the canonical grid.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuBetaGridStep n = 7 / 60 / ↑n
Instances For
The selected cells are those whose lower-left corner lies strictly below
the exact source line β = (1 - α) / 2.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuLogGridCells n = {q : Fin n × Fin n | MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n ↑q.2 < (1 - MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n ↑q.1) / 2}
Instances For
The finite-N upper-corner majorant on the selected canonical cells.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuLogGridMajorant n N = ∑ q ∈ MathlibNt.SieveTheory.LiuWeight.liuLogGridCells n, 1 / (1 - MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n (↑q.1 + 1) - MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n (↑q.2 + 1)) * MathlibNt.SieveTheory.PrimeReciprocalLogRectangle.primeReciprocalLogRectangle N (MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n ↑q.1) (MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n (↑q.1 + 1)) (MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n ↑q.2) (MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n (↑q.2 + 1))
Instances For
The fixed-grid logarithmic upper sum corresponding to
liuLogGridMajorant.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuLogGridUpperSum n = ∑ q ∈ MathlibNt.SieveTheory.LiuWeight.liuLogGridCells n, 1 / (1 - MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n (↑q.1 + 1) - MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n (↑q.2 + 1)) * MathlibNt.SieveTheory.PrimeReciprocalLogRectangle.logarithmicRectangleMass (MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n ↑q.1) (MathlibNt.SieveTheory.LiuWeight.liuAlphaGridPoint n (↑q.1 + 1)) (MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n ↑q.2) (MathlibNt.SieveTheory.LiuWeight.liuBetaGridPoint n (↑q.2 + 1))
Instances For
The exact root-free source condition p₁ p₂² ≤ N becomes the triangular
inequality α + 2β ≤ 1 in logarithmic coordinates.
Every selected cell has its upper-right corner strictly below the kernel
singularity α + β = 1.
Every Liu source pair belongs to a selected canonical cell. The natural ceiling construction handles points on upper grid boundaries without changing the source's strict-lower/non-strict-upper convention.
The canonical selected grid majorizes the full finite Liu logarithmic kernel sum.
For every fixed positive grid size, the finite-N majorant tends to its
logarithmic upper sum.
Eventual epsilon form of fixed canonical-grid convergence.
Threshold form of fixed canonical-grid convergence.