Block-L¹ weighted primitive consumers for the production Vaughan rows #
The analytic hypotheses in this file are block-local first-moment estimates for
exactly the production Type-I and Type-II coefficients. The finite consumer
converts d / φ(d) to the AP normalization on each block, reindexes a disjoint
finite block partition exactly, and then uses only the two scalar geometric
ledgers. The small lane is the production coefficient at
standardBVBalancedSmallCutoff, hence is retained and paid through its square
ledger plus high-conductor Cauchy. The former v = min N 1 path remains only
as an explicitly named compatibility wrapper.
The block-local d / φ(d) first moment, with the exact production prefix
amplitude.
Equations
- AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean a N S = ∑ d ∈ S, ↑d / ↑d.totient * ∑ ψ : AnalyticNumberTheory.LargeSieve.PrimitiveCharacter d, AnalyticNumberTheory.LargeSieve.primitivePrefixAmplitude a N d ψ
Instances For
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AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean_nonneg · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.apNormalizedPrimitiveMeanOn_le_inv_mul_blockWeighted · compiled type and proof/definition references.
Exact finite reindexing through a disjoint block partition.
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AnalyticNumberTheory.LargeSieve.apNormalizedPrimitiveMeanOn_eq_sum_blocks · compiled type and proof/definition references.
The complete finite block-L¹ consumer. A block estimate at the classical
N + (2i)²√N scale pays the AP mean by 1/i; summing uses exactly the two
geometric ledgers and nothing analytic.
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AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean_to_highMean · compiled type and proof/definition references.
Exact production Type-I specialization of the generic finite consumer.
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AnalyticNumberTheory.LargeSieve.productionTypeI_blockWeighted_to_highMean · compiled type and proof/definition references.
Exact production Type-II specialization, retaining the production hyperbolic Vaughan coefficient.
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AnalyticNumberTheory.LargeSieve.productionTypeII_blockWeighted_to_highMean · compiled type and proof/definition references.
Chosen exponents for paying a fixed block/shell logarithmic loss.
Equations
- AnalyticNumberTheory.LargeSieve.standardBVBlockL1ConductorExponent A loss = 2 * (A + loss + 1)
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AnalyticNumberTheory.LargeSieve.standardBVBlockL1ConductorExponent · compiled type and proof/definition references.
Equations
- AnalyticNumberTheory.LargeSieve.standardBVBlockL1ModulusExponent A loss = max (A + 3) (A + loss)
Instances For
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AnalyticNumberTheory.LargeSieve.standardBVBlockL1ModulusExponent · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.standardBVBlockL1_margin_B · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.standardBVBlockL1_loss_le_C · compiled type and proof/definition references.
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AnalyticNumberTheory.LargeSieve.standardBVBlockL1_loss_le_B · compiled type and proof/definition references.
Scalar payment for the block analytic input. The choices satisfy both
C ≥ A+loss and B ≥ A+loss; after the geometric block sum the two physical
scales are bounded by 10 N/log(N)^A.
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AnalyticNumberTheory.LargeSieve.standardBVBlockL1_scales_payable · compiled type and proof/definition references.
Canonical envelope-free production Type-I block mean-value predicate. The analytic source controls the literal block mean; the elementary Abel/conductor envelope is paid only by the downstream consumer.
Equations
- AnalyticNumberTheory.LargeSieve.ProductionTypeIBlockMeanValueBare N u v loss K G = ∀ i ∈ G.index, AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean (AnalyticNumberTheory.LargeSieve.vaughanTypeICoeff AnalyticNumberTheory.LargeSieve.vaughanUnitIntegerCoeff u v) N (G.cell i) ≤ K * Real.log ↑N ^ loss * (↑N + (2 * ↑i) ^ 2 * √↑N)
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AnalyticNumberTheory.LargeSieve.ProductionTypeIBlockMeanValueBare · compiled type and proof/definition references.
Canonical envelope-free production Type-II block mean-value predicate.
Equations
- AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValueBare N u v loss K G = ∀ i ∈ G.index, AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean (AnalyticNumberTheory.LargeSieve.vaughanTypeIICoeff AnalyticNumberTheory.LargeSieve.vaughanUnitIntegerCoeff u v) N (G.cell i) ≤ K * Real.log ↑N ^ loss * (↑N + (2 * ↑i) ^ 2 * √↑N)
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AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValueBare · compiled type and proof/definition references.
Legacy compatibility predicate with the Abel/conductor envelope already multiplied into the analytic hypothesis.
Equations
- AnalyticNumberTheory.LargeSieve.ProductionTypeIBlockMeanValue N u v loss P K G = ∀ i ∈ G.index, P * AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean (AnalyticNumberTheory.LargeSieve.vaughanTypeICoeff AnalyticNumberTheory.LargeSieve.vaughanUnitIntegerCoeff u v) N (G.cell i) ≤ K * Real.log ↑N ^ loss * (↑N + (2 * ↑i) ^ 2 * √↑N)
Instances For
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AnalyticNumberTheory.LargeSieve.ProductionTypeIBlockMeanValue · compiled type and proof/definition references.
The parallel production Type-II block mean-value theorem, retaining the existing exact hyperbolic Vaughan coefficient.
Equations
- AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValue N u v loss P K G = ∀ i ∈ G.index, P * AnalyticNumberTheory.LargeSieve.blockWeightedPrimitiveMean (AnalyticNumberTheory.LargeSieve.vaughanTypeIICoeff AnalyticNumberTheory.LargeSieve.vaughanUnitIntegerCoeff u v) N (G.cell i) ≤ K * Real.log ↑N ^ loss * (↑N + (2 * ↑i) ^ 2 * √↑N)
Instances For
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AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValue · compiled type and proof/definition references.
Legacy v = min N 1 block source, retained only for compatibility with
callers of the former degenerate small-lane assembler.
Equations
- AnalyticNumberTheory.LargeSieve.StandardBVProductionBlockL1WeightedLegacySource loss = ∀ (A : ℕ), have B := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ModulusExponent A loss; have C := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ConductorExponent A loss; ∃ (u : ℕ → 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) (AnalyticNumberTheory.LargeSieve.standardBVChosenSmallCutoff N) loss P K₁ G ∧ AnalyticNumberTheory.LargeSieve.ProductionTypeIIBlockMeanValue N (u N) (AnalyticNumberTheory.LargeSieve.standardBVChosenSmallCutoff N) loss P K₂ G
Instances For
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AnalyticNumberTheory.LargeSieve.StandardBVProductionBlockL1WeightedLegacySource · compiled type and proof/definition references.
Exact block analytic input on the canonical production dyadic geometry.
Type-I and Type-II use the same moving u,v, and the production v is the
balanced cube-root cutoff. No finite partition or geometric-ledger premise is
exposed.
Equations
- AnalyticNumberTheory.LargeSieve.StandardBVProductionBlockL1WeightedSource loss = ∀ (A : ℕ), have B := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ModulusExponent A loss; have C := AnalyticNumberTheory.LargeSieve.standardBVBlockL1ConductorExponent A loss; ∃ (u : ℕ → ℕ) (v : ℕ → ℕ), v = AnalyticNumberTheory.LargeSieve.standardBVBalancedSmallCutoff ∧ ∃ (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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AnalyticNumberTheory.LargeSieve.StandardBVProductionBlockL1WeightedSource · compiled type and proof/definition references.
Compatibility assembler for the former degenerate v = min N 1 source.
New production code must use
standardBVHighTypeITypeIIHybridChosenSource_of_blockL1Weighted.
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AnalyticNumberTheory.LargeSieve.standardBVHighTypeITypeIIHybridChosenSource_of_blockL1Weighted_legacy · compiled type and proof/definition references.
Consume the actual high-conductor square payment for any coefficient. The factor three is the existing ledger reserve, not a new triangle bound. Only the target needs to be nonnegative; the multiplier may be signed.
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AnalyticNumberTheory.LargeSieve.apNormalizedPrimitiveMeanOn_high_le_of_square_payment · compiled type and proof/definition references.
Production block-L¹ chosen assembler. Type-I and Type-II use one shared
pair u,v, with v = standardBVBalancedSmallCutoff; their block first moments
are paid by the block geometry, while the retained balanced small mean is paid
by standardBVChosenSmall_squareLedger_payable followed by the existing
high-conductor weighted Cauchy inequality.
Inspect dependencies
AnalyticNumberTheory.LargeSieve.standardBVHighTypeITypeIIHybridChosenSource_of_blockL1Weighted · compiled type and proof/definition references.
The common quadratic envelope used by chosen Type-I/II payments and by
bare block sources. The modulus is the actual Pan cutoff, including Q = 0.
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AnalyticNumberTheory.LargeSieve.productionAbelConductorEnvelope_le_logPow_two · compiled type and proof/definition references.
The production Abel/conductor envelope costs at most five logarithms. The proof actually gives a quadratic logarithm; exponent five is frozen as a stable reserve for canonical bare block sources.
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AnalyticNumberTheory.LargeSieve.productionAbelConductorEnvelope_le_logPow_five · compiled type and proof/definition references.
Canonical bare block source. Its analytic hypotheses contain no Abel/conductor factor. The selected exponents reserve the fixed five-log consumer payment.
Equations
- AnalyticNumberTheory.LargeSieve.StandardBVProductionBlockL1BareSource 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), v = AnalyticNumberTheory.LargeSieve.standardBVBalancedSmallCutoff ∧ ∃ (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
Instances For
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AnalyticNumberTheory.LargeSieve.StandardBVProductionBlockL1BareSource · compiled type and proof/definition references.
Multiplying a bare Type-I block estimate by an envelope bounded by five logarithms shifts the loss by exactly five.
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AnalyticNumberTheory.LargeSieve.productionTypeIBlockMeanValue_of_bare_logPow_five · compiled type and proof/definition references.
Type-II version of the fixed five-log consumer payment.
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AnalyticNumberTheory.LargeSieve.productionTypeIIBlockMeanValue_of_bare_logPow_five · compiled type and proof/definition references.
Consumer-side bridge: a canonical bare source becomes the balanced weighted source after the fixed loss translation.
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AnalyticNumberTheory.LargeSieve.standardBVProductionBlockL1WeightedSource_of_bare · compiled type and proof/definition references.
The canonical envelope-free block source is connected to the chosen high Standard-BV node; all envelope loss is paid in the consumer above.
Inspect dependencies
AnalyticNumberTheory.LargeSieve.standardBVHighTypeITypeIIHybridChosenSource_of_blockL1Bare · compiled type and proof/definition references.