The complete endpoint remainder after transporting the cubic endpoint from
yr = D^(1/3) to zr = D^(1/s). In contrast with the legacy natural-cutoff
wrapper, both analytic cutoff coordinates are the exact real roots.
Equations
- MathlibNt.SieveTheory.caseIIRoundedTransportErr S H N D yr zr d Δ σ C K B0 s = B0 + MathlibNt.SieveTheory.SwitchingPrinciple.suzukiVProduct S zr * (3 / s * (K / Real.log yr) * MathlibNt.SieveTheory.SuzukiFiniteContinuousLayers.finiteSourceLayer 1 2 N 3 + 3 / s * (1 + K / Real.log yr) * MathlibNt.SieveTheory.caseIIEndpointSigma11 K N D σ + 3 / s * (1 + K / Real.log yr) * MathlibNt.SieveTheory.caseIIEndpointQD H N D d Δ σ C K)
Instances For
Inspect dependencies
MathlibNt.SieveTheory.caseIIRoundedTransportErr · compiled type and proof/definition references.
Sharp source-native Case-II assembly when the target cutoff is the natural ceiling of the exact real power coordinate.
Inspect dependencies
MathlibNt.SieveTheory.caseII_total_le_concrete_finiteSourceLayer_add_rawBase_natCeil · compiled type and proof/definition references.
Double-rounded sharp Case-II endpoint transport.
The natural cutoffs are y = ceil(D^(1/3)) and z = ceil(D^(1/s)).
Dimension-one transport and the logarithmic ratio are carried out only at the
exact real roots. The two Euler products are then returned exactly to their
natural-ceiling cutoffs; no equality between a cast natural cutoff and a real
root is assumed.
Inspect dependencies
MathlibNt.SieveTheory.caseII_total_le_from_caseI_endpoint_explicit_rawBase_natCeil · compiled type and proof/definition references.