Original Eq19 allocation: pair second, natural Mobius fourth, derivative fourth.
Equations
- AnalyticNumberTheory.LargeSieve.eq19BetaLinearCoefficient x L level B k H D Q = √(9 * AnalyticNumberTheory.LargeSieve.chen1973Lemma6Eq19SharpConstant * AnalyticNumberTheory.LargeSieve.chen1973Lemma6Eq19I x L level / Real.log ↑x ^ 2 * (↑Q + ↑(B * 2 ^ k) / ↑D) * ↑(B * 2 ^ k) ^ (1 - 2 * AnalyticNumberTheory.LargeSieve.chen1973Lemma6Beta x)) * √√(AnalyticNumberTheory.LargeSieve.chen1973Lemma6Eq19I x L level * (AnalyticNumberTheory.LargeSieve.chen1973Lemma6Eq19SharpConstant * (↑Q + ↑(H * H) / ↑D) * (1 + Real.log ↑(H * H)) ^ 4)) * √√(AnalyticNumberTheory.LargeSieve.chen1973Lemma6Eq20BetaDerivativeCoefficient x L level D Q)
Instances For
The corrected beta integral at any H; the height is not an Eq20 complement.
The large-Y cutoff is a consequence of the actual carrier, never an extra assumption.
Empty shells give the literal zero numerator and corrected integral.
The source cut gives the cap required by the already verified alpha endpoint.
Uniform subpower control of the printed exponential, with threshold before level.
Upper height budget at the actual ceil, not the obsolete W-height.
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Algebraic joining of pair², S⁴ and L'⁴ preserves the square-root conductor scale.
Source-faithful scalar numerator coefficient at the printed height.
Both conductor and nonempty-pair scales retain a strict power margin.
Printed-height beta smallness for every source cell; no hypothesis bounds Y.
The positive Eq19 cell, now with both actual corrected integrals paid.