The only analytic input below is the explicitly conditional unweighted Pan (1975) Theorem 2 specialization for the actual convolution error. The weight payment is modern finite Cauchy, as in Maynard Lemma 5.2 (5.19)--(5.20). It is not an application of ordinary prime Bombieri--Vinogradov to a convolution.
Exactly the same interval, normalization and residue maximum as the weighted source.
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- MathlibNt.SieveTheory.LiuWeight.liuPanActualError κ N B q = MathlibNt.SieveTheory.LiuWeight.liuMainPanCoprimeIntervalMaxL (MathlibNt.SieveTheory.LiuWeight.liuLogarithmicIntegral κ) N (MathlibNt.SieveTheory.LiuWeight.liuPanSourceIntervalLower N B) (MathlibNt.SieveTheory.LiuWeight.liuPanSourceIntervalUpper N) q (MathlibNt.SieveTheory.LiuWeight.liuWeight N (MathlibNt.SieveTheory.LiuWeight.liuSourceZ10 N) (MathlibNt.SieveTheory.LiuWeight.liuSourceY3 N))
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The actual source mass with both μ² and 3^ω removed, not a prime discrepancy.
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Still-unproved analytic input: a Liu specialization of Pan (1975), Theorem 2. κ is fixed before U; U is the saving exponent, not the cutoff exponent B.
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A single global ninth-moment constant is fixed before κ,N,B. No distribution assumption or extra envelope hypothesis remains in this finite theorem.