Chen 1973, Lemma 6: source spine for the M₂ bound #
This file follows printed pp. 119--123, equations (12)--(21). It freezes the
actual M₂ from Chen1973Lemma5SwitchedTripleSource, the literal prime-pair
and conductor dyadic carriers, and the finite reindexing behind (13).
The analytic estimates are deliberately not hidden in a conclusion-shaped record. The terminal theorem takes separately named hypotheses with the exact roles of displayed equations (12), (19), (20), and (21), plus the final logarithmic absorption. All finite carrier identities are proved here.
The source's finite Dirichlet polynomial is represented by Finset.Icc 1 H
(in natural order). This matters on the β = 1/2 + 1/log x line: no
conditionally convergent infinite reordering is introduced.
Source ledger (verified directly on printed pp. 119--123):
- (12) is
M₂ ≪ (log x)^6 max_{1<m≤x^(1/2)} N_m. - (13) uses
0≤l≤I₁,0≤k≤I₂, low conductors1<d≤(log x)^100, high cells2^(l-1)(log x)^100<d≤2^l(log x)^100, and pair cellsx^(13/30)2^k<p₁p₂≤x^(13/30)2^(k+1). - (14) is the second moment for
1-LS; (15) is the fourth moment of the natural-order polynomialS(H,β+iv,χ); (16) is the algebraicL'/Lsplit; (17) has the printed second prefactorx^(1/2). - (18) bounds
3^ν(d)on squarefree conductors. Equations (19) and (20) giveN_m^(l,k) ≪ x/(log x)^20; in the second case the printed choice isH=max(2^(2l-k)x^(-13/30)(log x)^400 I_{l,x}, x^(1/2-ε)). - (21) treats the low-conductor
l=0cells using the primitive-character zero-free line. Finally (12), (13), and (19)--(21) yield the printedM₂ ≪ x/(log x)^2.01.
The p. 120 polynomial S(H,s,χ)=∑_{n=1}^H μ(n)χ(n)n⁻ˢ, with the
natural-number order made literal.
Equations
- AnalyticNumberTheory.LargeSieve.chen1973Lemma6MobiusPartialSum H s χ = ∑ n ∈ Finset.Icc 1 H, ↑(ArithmeticFunction.moebius n) * ↑χ ↑n / ↑n ^ s
Instances For
The exact finite square before collecting equal products into the source's
coefficient j(n). Both indices are natural-order finite partial sums, so this
identity is valid equally on the Re(s)≤1 line used in (15).
A dyadic shell with the source convention B·2^k < size ≤ B·2^(k+1).
Equations
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The complete dyadic hull covered by levels 0,…,K.
Equations
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Exact finite union of the printed dyadic shells.
The printed shells are pairwise disjoint; hence finite sums may be reindexed without multiplicity.
Exact sum reindexing over the source dyadic hull.
The literal p. 119 prime-pair shell
x^(13/30)2^k < p₁p₂ ≤ x^(13/30)2^(k+1), represented by an honest natural
base cutoff B; the real-power correspondence is stated separately below.
Equations
- AnalyticNumberTheory.LargeSieve.chen1973Lemma6PrimePairShell x B k m = AnalyticNumberTheory.LargeSieve.chen1973Lemma6DyadicShell ({pp ∈ AnalyticNumberTheory.LargeSieve.chen1973Lemma5PrimePairs x | (pp.1 * pp.2).Coprime m}) (fun (pp : ℕ × ℕ) => pp.1 * pp.2) B k
Instances For
The conductor blocks in (13): level zero is 1<d≤L; level l+1 is
2^l L<d≤2^(l+1)L.
Equations
- AnalyticNumberTheory.LargeSieve.chen1973Lemma6ConductorBlock x L level = if level = 0 then {d ∈ Finset.Ioc 1 L | d.Coprime x ∧ Squarefree d} else {d ∈ AnalyticNumberTheory.LargeSieve.chen1973Lemma6DyadicShell (Finset.Ioc 1 (L * 2 ^ level)) id L (level - 1) | d.Coprime x ∧ Squarefree d}
Instances For
The exact p. 119 summand of N_m, with Chen's Möbius/3^ν weight,
primitive-character sum, reciprocal logarithm, and actual semiprime carrier.
Phi d χ y is the displayed contour kernel Φ(y,χ) defined at the start of
Lemma 6; it is not an arbitrary coefficient sequence on integers.
Equations
- AnalyticNumberTheory.LargeSieve.chen1973Lemma6NmBlock x L level B k m Phi = ∑ d ∈ AnalyticNumberTheory.LargeSieve.chen1973Lemma6ConductorBlock x L level, |↑(ArithmeticFunction.moebius d)| * 3 ^ d.primeFactors.card / ↑d * ‖∑ χ : AnalyticNumberTheory.LargeSieve.PrimitiveCharacter d, star (↑χ ↑x) * ∑ pp ∈ AnalyticNumberTheory.LargeSieve.chen1973Lemma6PrimePairShell x B k m, ↑(Real.log (↑x / (↑pp.1 * ↑pp.2)))⁻¹ * Phi d χ (↑x / (↑pp.1 * ↑pp.2)) * ↑χ ↑(pp.1 * pp.2)‖
Instances For
The complete right side of source equation (13).
Equations
- AnalyticNumberTheory.LargeSieve.chen1973Lemma6DyadicMajorant x L I1 B I2 m Phi = ∑ level ∈ Finset.range (I1 + 1), ∑ k ∈ Finset.range (I2 + 1), AnalyticNumberTheory.LargeSieve.chen1973Lemma6NmBlock x L level B k m Phi
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1≤l≤I₁ cells in the first two ranges treated by source equation (19).
Equations
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1≤l≤I₁ cells in the complementary range treated by source equation (20).
Equations
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Transparent source chain (12), (13), (19)--(21) to Lemma 6's terminal
2.01 bound. Each analytic input is a concrete inequality about the displayed
quantity; there is no Prop wrapper carrying the conclusion.