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MathlibNt.SieveTheory.LinearSieve.Suzuki.SuzukiProposition118FinitePrefixPairing

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.

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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
Instances For
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    MathlibNt.SieveTheory.suzukiProposition118SourceQTerminal · compiled type and proof/definition references.

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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.