Rank-one rectangular primitive L¹ means #
This leaf separates the elementary rectangular part of a Type-II first moment from the genuinely hyperbolic prefix problem. A rank-one rectangle is paid by two one-dimensional weighted primitive large sieves and one Cauchy--Schwarz inequality. The sole remaining interface says that an actual collected Vaughan hyperbolic shell is dominated by finitely many such rectangles.
This module is intentionally not imported by a canonical facade.
Weighted primitive first moment of a rank-one rectangular character sum. The conductor set is explicit so the same theorem applies to one production conductor block.
Equations
- AnalyticNumberTheory.LargeSieve.rankOneRectangularWeightedPrimitiveMean a b Ma Mb Na Nb S = ∑ q ∈ S, ↑q / ↑q.totient * ∑ χ : AnalyticNumberTheory.LargeSieve.PrimitiveCharacter q, ‖∑ m ∈ Finset.Icc (Ma + 1) (Ma + ↑Na), a m * ↑χ ↑m‖ * ‖∑ n ∈ Finset.Icc (Mb + 1) (Mb + ↑Nb), b n * ↑χ ↑n‖
Instances For
The elementary rectangular theorem. After flattening the finite dependent
family (q,χ), Cauchy gives two square ledgers; each is exactly one invocation
of the one-dimensional weighted primitive large sieve.
Unsquared form convenient for finite shell assembly.
The unique analytic residual: separation of one actual hyperbolic collected shell into finitely many rank-one rectangles. Everything after this interface is the proved rectangular theorem above and finite summation.
Equations
- AnalyticNumberTheory.LargeSieve.VaughanTypeIIHyperbolicSeparation N u v k l S left right leftStart rightStart leftLength rightLength = (AnalyticNumberTheory.LargeSieve.blockWeightedVaughanActualCollectedShellMean N u v k l S ≤ ∑ i : ι, AnalyticNumberTheory.LargeSieve.rankOneRectangularWeightedPrimitiveMean (left i) (right i) (leftStart i) (rightStart i) (leftLength i) (rightLength i) S)
Instances For
A separated actual shell is paid solely by the two one-dimensional large sieves for each rank-one rectangle.
Connection to the actual Vaughan fixed-conductor-block L¹ mean. The only
premise not discharged by existing finite decomposition or one-dimensional
large sieve is VaughanTypeIIHyperbolicSeparation, once for each active shell.