Proposition 11.8 from finite full-layer prefixes #
The prefix below follows the production source definition exactly. Above the
source boundary it contains the first m odd and first m even source layers;
below the boundary it uses the finite amplitude A_m / s. Thus the initial
history is part of the prefix, rather than being silently replaced by the
out-of-domain values of the recursive layer formula.
The genuine full source prefix, including its prescribed initial history.
Equations
Instances For
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MathlibNt.SieveTheory.suzukiProposition118SourceQPrefix · compiled type and proof/definition references.
Only the last even layer is left after the finite weighted source equations
telescope. It starts at the true delayed source boundary s=3; below that
point the finite initial history closes the telescope exactly.
Equations
- MathlibNt.SieveTheory.suzukiProposition118SourceQTerminal m s = if 3 < s then MathlibNt.SieveTheory.SuzukiFiniteContinuousLayers.suzukiLayer 1 2 (2 * m) (s - 1) else 0
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MathlibNt.SieveTheory.suzukiProposition118SourceQTerminal · compiled type and proof/definition references.
The corresponding single-terminal-layer pairing residual.
Equations
Instances For
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MathlibNt.SieveTheory.suzukiProposition118SourceQTerminalPairingResidual · compiled type and proof/definition references.
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MathlibNt.SieveTheory.suzukiLayer_weighted_eq_integral_to_upper · compiled type and proof/definition references.
Away from its parity threshold, the weighted recursive layer has the literal source derivative. No infinite sum is differentiated.
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MathlibNt.SieveTheory.hasDerivAt_weighted_suzukiLayer_of_threshold_lt · compiled type and proof/definition references.