The narrow conductor-local primitive large-sieve input #
The full-cutoff primitive large sieve bounds a retained conductor block by the
same L + Q² constant as the full block. That statement cannot create the
R⁻¹ diagonal needed after deleting conductors d ≤ R. This file therefore
freezes the missing analytic input at the square-ledger level, before any
unsquared high mean is formed.
Coefficient energy of one primitive prefix row.
Equations
- AnalyticNumberTheory.LargeSieve.conductorLocalRowEnergy b M L = ∑ n ∈ Finset.Icc (M + 1) (M + ↑L), ‖b n‖ ^ 2
Instances For
The precise missing analytic strengthening of the primitive prefix-maximal large sieve. It is a square-ledger statement for an arbitrary coefficient row. In particular it neither mentions nor assumes a Vaughan high mean.
The L/R diagonal is the only new information relative to the existing
full-cutoff theorem; the Q² lane is unchanged.
Equations
- AnalyticNumberTheory.LargeSieve.ConductorLocalPrimitiveLargeSieve K = ∀ (R Q L : ℕ) (b : ℤ → ℂ) (M : ℤ), 0 < R → 0 < Q → (AnalyticNumberTheory.LargeSieve.highConductorHarmonicTail R Q * AnalyticNumberTheory.LargeSieve.highConductorPrimitiveSquareLedger R Q fun (d : ℕ) (χ : AnalyticNumberTheory.LargeSieve.PrimitiveCharacter d) => √(AnalyticNumberTheory.LargeSieve.primitiveCharacterPrefixMaxSquare b M L d χ)) ≤ K ^ 2 * ↑(L.log2 + 1) ^ 2 * (↑L * AnalyticNumberTheory.LargeSieve.conductorLocalRowEnergy b M L / ↑R + ↑Q ^ 2 * AnalyticNumberTheory.LargeSieve.conductorLocalRowEnergy b M L)
Instances For
Square-ledger extraction. Once the actual row geometry supplies
L * energy ≤ N² and energy ≤ N, the local primitive large sieve gives the
required N/√R + Q√N scale.