AP-normalized direct Vaughan assembly #
This module is the direct L¹ route with the literal arithmetic-progression
weight 1 / φ(q). The historical q / φ(q) unsquared mean remains available
only as a compatibility majorant in VaughanDirectL1Physical.
AP-normalized Type-II direct Vaughan mean.
Equations
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AP-normalized small-range direct Vaughan mean.
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Weighted Cauchy in the modulus variable. The reciprocal square roots
produce the harmonic factor, while the second factor is exactly the usual
q / φ(q) square-large-sieve ledger. Thus q / φ(q) appears only inside the
proved square estimate, never as the direct unsquared mean.
Vaughan's exact three-piece identity assembled directly in the AP-normalized primitive L¹ mean.
Strong conductor transport. The exact reciprocal-totient conductor bound
lands on the AP-normalized primitive mean, with no q / φ(q) inflation.
All nonprincipal characters transported to the AP-normalized primitive mean. The change-of-level correction remains explicit.
Largest short-variable scale occurring in the two Type-I lanes.
Equations
- AnalyticNumberTheory.LargeSieve.vaughanTypeIShortScale u v = max u (u * v)
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AP-normalized Type-I physical-scale input, retaining the exact
Q*sqrt(N*D) dependence of the shell square ledger.
Equations
- AnalyticNumberTheory.LargeSieve.VaughanDirectAPNormalizedTypeIInput N Q u v K logPay = (AnalyticNumberTheory.LargeSieve.apNormalizedVaughanTypeIMean N Q u v ≤ K * logPay * (↑N + ↑Q ^ 2 * √↑N))
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AP-normalized Type-II physical-scale input.
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Physical direct assembly through the AP-normalized primitive mean. In
particular, conductor transport never invokes the compatibility
q / φ(q) unsquared mean.