The actual boundary mask depends only on the long coordinate.
Equations
- G12FineGrid.boundaryMask ρ N ε k m = (m ∈ Finset.Ioc (G12FineGrid.longLower ρ k) (G12FineGrid.longUpper ρ N k) ∧ ¬G12FlexibleRectangle.longOK N ε (G12FineGrid.shortLower ρ N k) (G12FineGrid.shortUpper ρ N k) m)
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G12FineGrid.boundaryMask · compiled type and proof/definition references.
The original normalized coefficient, with only a long-variable mask.
Equations
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G12FineGrid.boundaryCoefficient · compiled type and proof/definition references.
Original PiLi endpoints clipped at the actual short-cell endpoints. Coprimality is retained on the short side, never asserted to inherit SW.
Equations
- G12FineGrid.boundaryWindow ρ N ε k m = {r ∈ Finset.range (N + 1) | Nat.Prime r ∧ r.Coprime N ∧ max (MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11PiLiLo N ε m) ↑(G12FineGrid.shortLower ρ N k) < ↑r ∧ ↑r ≤ min (MathlibNt.SieveTheory.LiLiuOnePlusOneNine.GoldbachBig.goldbachG11PiLiHi N m) ↑(G12FineGrid.shortUpper ρ N k)}
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G12FineGrid.boundaryWindow · compiled type and proof/definition references.
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G12FineGrid.boundaryMask_iff · compiled type and proof/definition references.
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G12FineGrid.boundaryCoefficient_bounds · compiled type and proof/definition references.
Coprimality removes the apparent closed product endpoint in PiLiHi.
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G12FineGrid.motherCell_window_iff · compiled type and proof/definition references.
Literal finite-set representation, with the original active support.
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G12FineGrid.boundaryCell_eq_masked_window · compiled type and proof/definition references.
Exact weighted identity for any test: AP, coprimality, or output-prime. No cancellation is lost and the physical coefficient is unchanged.
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G12FineGrid.boundaryCell_weighted_window · compiled type and proof/definition references.