Faithful Vaughan small cutoff for a fixed global modulus cutoff Q.
The explicit zero branch records the safe interpretation at Q = 0.
Equations
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Ordinary primitive prefix-maximal large sieve for an arbitrary small cutoff.
No comparison of coefficient values is used: the dependence on v enters only
through the established small-coefficient energy bound.
The complete weighted small square ledger is paid for any eventually balanced-bounded cutoff, with no coefficient zeroing.
Weighted adaptive source used as the intermediate output of the five-log envelope payment. Its only cutoff restriction is the balanced upper bound.
Equations
- AnalyticNumberTheory.LargeSieve.StandardBVProductionAdaptiveBlockL1WeightedSource loss = ∀ (A : ℕ), have B := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ModulusExponent A loss; have C := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ConductorExponent A loss; ∃ (u : ℕ → ℕ) (v : ℕ → ℕ), (∀ (N : ℕ), v N ≤ AnalyticNumberTheory.LargeSieve.standardBVBalancedSmallCutoff N) ∧ ∃ (K₁ : ℝ) (K₂ : ℝ), 0 < K₁ ∧ 0 < K₂ ∧ ∀ᶠ (N : ℕ) in Filter.atTop, have Q := MathlibNt.SieveTheory.LiuWeight.panModulusCutoff N ↑B; have P := 4 * AnalyticNumberTheory.LargeSieve.discreteAbelAmplifierPrefixMax N * AnalyticNumberTheory.LargeSieve.conductorHarmonicFactor Q ^ 2; ∀ (hR : 0 < AnalyticNumberTheory.LargeSieve.logConductorThreshold N C), have G := AnalyticNumberTheory.LargeSieve.productionConductorBlockGeometry N Q C hR; AnalyticNumberTheory.LargeSieve.ProductionTypeIBlockMeanValue N (u N) (v N) loss P K₁ G ∧ AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValue N (u N) (v N) loss P K₂ G
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Adaptive bare block source. Since the existential pair is selected after
A, both cutoffs may vary with A and N; no equality to a canonical cutoff
is imposed, only v N ≤ the balanced cube-root cutoff.
Equations
- AnalyticNumberTheory.LargeSieve.StandardBVProductionAdaptiveBlockL1BareSource loss = ∀ (A : ℕ), have paidLoss := loss + 5; have B := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ModulusExponent A paidLoss; have C := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ConductorExponent A paidLoss; ∃ (u : ℕ → ℕ) (v : ℕ → ℕ), (∀ (N : ℕ), v N ≤ AnalyticNumberTheory.LargeSieve.standardBVBalancedSmallCutoff N) ∧ ∃ (K₁ : ℝ) (K₂ : ℝ), 0 < K₁ ∧ 0 < K₂ ∧ ∀ᶠ (N : ℕ) in Filter.atTop, have Q := MathlibNt.SieveTheory.LiuWeight.panModulusCutoff N ↑B; ∀ (hR : 0 < AnalyticNumberTheory.LargeSieve.logConductorThreshold N C), have G := AnalyticNumberTheory.LargeSieve.productionConductorBlockGeometry N Q C hR; AnalyticNumberTheory.LargeSieve.ProductionTypeIBlockMeanValueBare N (u N) (v N) loss K₁ G ∧ AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValueBare N (u N) (v N) loss K₂ G
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Production block-L¹ chosen assembler. Type-I and Type-II use one shared
pair u,v, with only v N ≤ standardBVBalancedSmallCutoff N; their block first moments
are paid by the block geometry, while the retained small mean is paid
by standardBVSmall_squareLedger_payable_of_le_balanced followed by the existing
high-conductor weighted Cauchy inequality.
Five-log envelope payment followed by the generalized small-lane payment.