Combined inverse-log discrepancy for Liu's Pan endpoint #
The Type I endpoint, Type II endpoint, and complete signed-main kernel are
recombined before taking an absolute value. Vaughan's finite identity then
identifies this expression with the source-weighted Λ / log discrepancy.
The already separated prime-power correction remains on its own power-saving
scale.
The older componentwise contracts are intentionally left unchanged. Their degenerate or conductor-one endpoint behavior does not prove the combined estimate introduced here.
Exact finite combination #
The Type I endpoint, Type II endpoint, and complete signed main, combined inside one absolute value before any analytic estimate is applied.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuPanCombinedInverseLogDiscrepancy main y X q l f u v = |((AnalyticNumberTheory.Sieve.panPieceSum y X q l f fun (y q l : ℕ) => AnalyticNumberTheory.Sieve.apV1 y q l u / Real.log ↑y) + AnalyticNumberTheory.Sieve.panPieceSum y X q l f fun (y q l : ℕ) => AnalyticNumberTheory.Sieve.apV3 y q l u v / Real.log ↑y) + MathlibNt.SieveTheory.LiuWeight.liuPanSignedMainSum main y X q l f u v|
Instances For
Vaughan's logarithmic identity recombines the three endpoint terms into
the exact source-weighted Λ / log discrepancy.
Source-facing specialization of the exact combined identity.
Maximum of the exact combined discrepancy over canonical reduced residues.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuPanCombinedInverseLogMaxL main y X q f u v = if h : (AnalyticNumberTheory.Sieve.unitResidues q).Nonempty then (Finset.image (fun (l : ℕ) => MathlibNt.SieveTheory.LiuWeight.liuPanCombinedInverseLogDiscrepancy main y X q l f u v) (AnalyticNumberTheory.Sieve.unitResidues q)).max' ⋯ else 0
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Maximum of the exact combined discrepancy over y ≤ x.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuPanCombinedInverseLogMaxY main X q x f u v = (Finset.image (fun (y : ℕ) => MathlibNt.SieveTheory.LiuWeight.liuPanCombinedInverseLogMaxL main y X q f u v) (Finset.range (x + 1))).max' ⋯
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Modulus one uses its unique canonical residue 0.
The modulus-one y-maximum retains the unique residue 0.
Exact correction separation and maxima #
Only the prime-power correction is separated after the three principal endpoint terms have been recombined.
The canonical residue maximum inherits the exact combined-plus-correction bound.
The two nested maxima preserve the combined-before-absolute-value route.
Source-family analytic input #
The weighted combined inverse-log average for Liu's source at a fixed N.
Equations
- MathlibNt.SieveTheory.LiuWeight.liuMainPanCombinedInverseLogAverage kappa N B u v = ∑ q ∈ Finset.range (MathlibNt.SieveTheory.LiuWeight.panModulusCutoff N B + 1), ↑(ArithmeticFunction.moebius q) ^ 2 * 3 ^ q.primeFactors.card * MathlibNt.SieveTheory.LiuWeight.liuPanCombinedInverseLogMaxY (MathlibNt.SieveTheory.LiuWeight.liuLogarithmicIntegral kappa) N q N (MathlibNt.SieveTheory.LiuWeight.liuWeight N (MathlibNt.SieveTheory.LiuWeight.liuSourceZ10 N) (MathlibNt.SieveTheory.LiuWeight.liuSourceY3 N)) u v
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The fixed-source combined inverse-log estimate.
Equations
- MathlibNt.SieveTheory.LiuWeight.LiuMainPanCombinedInverseLogBoundAt kappa N A B C u v = (MathlibNt.SieveTheory.LiuWeight.liuMainPanCombinedInverseLogAverage kappa N B u v ≤ C * ↑N / Real.log ↑N ^ A)
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The source-family combined estimate, with f_N chosen inside the final
universal quantifier over N.
Equations
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The source Pan average is bounded by the combined discrepancy and only the separately controlled prime-power correction.
Fixed-N eqn-r consumer. The combined inverse-log estimate and the
prime-power power saving remain on their distinct scales.
Source-family and little-oh consumers #
The source-family combined estimate and the proved source prime-power
endpoint give the exact eqn-r majorant with three distinct scales.
A cubic inverse-log bound is negligible relative to N / log(N)^2.
The exact Liu eqn-r distribution majorant is
o(N / log(N)^2) under the combined source-family predicate. The proved
prime-power power saving and the established R₁ estimate are used only at
their own scales.
Consequently, every eventually admissible Selberg lambda family has its actual signed remainder negligible on the downstream main scale.