The explicit arithmetic loss; this is not an input bound on the energy.
Equations
- MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.directPayMainLoss κ δ ρ Cnonzero Cτ Cjoint Ca Ccoeff x a K F j = (Ccoeff * x ^ ρ * (Ccoeff * x ^ ρ)) ^ 2 * (Cnonzero * (Ca * ↑a.natAbs ^ δ)) * (16 * 2 ^ j 2 * 2 ^ j 3 * (2 ^ j 4) ^ 2) ^ κ * √(Cτ * Cjoint) * ↑(MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.mainRestrictedMax a K.1.2.1 (2 ^ (j 2 + 1)) (F / K.1.1) (2 ^ (j 0 + 1)) (2 ^ (j 4 + 1))) ^ δ * √(1 + Real.log (2 ^ (j 4 + 1)))
Instances For
Inspect dependencies
MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.directPayMainLoss · compiled type and proof/definition references.
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MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.directPayMainLoss_nonneg · compiled type and proof/definition references.
The literal joint mean pays the entire coefficient-pair length using F≤2T.
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MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.directPayMain_mean_le · compiled type and proof/definition references.
The q^(1/2+κ) factor is genuinely split, retaining q^κ in the explicit loss.
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MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.directPayMain_qpow · compiled type and proof/definition references.
Fully expanded actual energy. Both completion terms remain visible.
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MathlibNt.AnalyticNumberTheory.LargeSieve.LiLiuPrereqFouvry.directPayMain_energy_le · compiled type and proof/definition references.