The finite Euler product V(z) on the supported prime carrier.
Equations
- MathlibNt.SieveTheory.sourceDiscreteEuler S z = ∏ p ∈ MathlibNt.SieveTheory.SwitchingPrinciple.suzukiSupportedBelow S z, (1 - S.nu p)
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Suzuki's discrete V_n(D,z), with complete-chain source index n.
At n=1 this is exactly the one-prime terminal shell
p < D ∧ D ≤ p^3. For n+2, peeling the largest source prime gives the
source recurrence with level D/p, encoded exactly on naturals by
D ⌈/⌉ p. Index zero is deliberately zero: it is not a source layer.
Equations
- MathlibNt.SieveTheory.section14ExtendedV S 0 x✝¹ x✝ = 0
- MathlibNt.SieveTheory.section14ExtendedV S 1 x✝¹ x✝ = ∑ p ∈ MathlibNt.SieveTheory.SwitchingPrinciple.suzukiSupportedBelow S x✝ with p < x✝¹ ∧ x✝¹ ≤ p ^ 3, S.nu p * MathlibNt.SieveTheory.sourceDiscreteEuler S p
- MathlibNt.SieveTheory.section14ExtendedV S n.succ.succ x✝¹ x✝ = ∑ p ∈ MathlibNt.SieveTheory.SwitchingPrinciple.suzukiSupportedBelow S x✝, S.nu p * MathlibNt.SieveTheory.section14ExtendedV S (n + 1) (x✝¹ ⌈/⌉ p) p
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Exact one-prime source recurrence, valid for every positive predecessor index. No positivity or analytic hypothesis is used.
Exact support boundary for the exceptional source layer V₁. This is the
finite form used in Suzuki's Case I when s ≥ β+1 and β=2: z^3 ≤ D.
Source-selected indices 1 ≤ n ≤ N, n ≡ N (mod 2).
Equations
- MathlibNt.SieveTheory.sourceParityIndices N = {n ∈ Finset.Icc 1 N | n % 2 = N % 2}
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The positive-index tail, used to separate the exceptional V₁ term.
Equations
- MathlibNt.SieveTheory.sourceParityTailIndices N = {n ∈ Finset.Icc 2 N | n % 2 = N % 2}
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The finite discrete parity sum T_N(D,z).
Equations
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Exact parity recurrence for even source cutoff N. Since every selected
index is at least two, no terminal boundary term occurs.
For odd N, the only obstruction to the same recurrence is the source
base layer V₁; all higher selected layers reindex exactly.
Suzuki Case-I exact recurrence. For even N it is unconditional; for odd
N, the precise boundary hypothesis is the vanishing of V₁(D,z).
The concrete Case-I boundary z^3 ≤ D kills V₁, hence yields the exact
recurrence for both parities.
The normalized lower V_n(D,z)/V(z) written directly on the production
lower-boundary chain carrier. The terminal prime q is external to l, so
the complete source index is imposed by l.length + 1 = n.
Equations
- MathlibNt.SieveTheory.sourceDiscreteLowerBoundaryV S n D z = ∑ q ∈ MathlibNt.SieveTheory.SwitchingPrinciple.suzukiSupportedBelow S z, S.nu q * MathlibNt.SieveTheory.SwitchingPrinciple.suzukiSuffixRatio S z q * ∑ l ∈ MathlibNt.SieveTheory.LinearSieve.lowerRosserBoundaryChainsAtSourceIndex D q ({p ∈ MathlibNt.SieveTheory.SwitchingPrinciple.suzukiSupportedBelow S z | q < p}) n, (List.map (⇑S.nu) l).prod
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The recursive source layer at index two, fully expanded. This is the
strongest unconditional comparison datum with the lower boundary carrier: its
inner terminal shell is tested at the divided level D ⌈/⌉ p.
The chain-based lower slice at index two, fully expanded. In contrast to
section14ExtendedV_two_eq_recursiveCarrier, the stored prime is tested by
p < D, while the terminal prime q occurs only in the cubic crossing test
D ≤ p*q^3. Thus the two definitions do not have the same base carrier.
The base carriers are genuinely different, already on prime-shaped data:
with stored prime p = 5, terminal prime q = 2, and level D = 9, the
chain predicate holds but the recursive divided-level predicate does not.
A lower-boundary source slice is supported only at even complete-chain indices.
Exact identification of the direct source-index slice with the existing
production lower layer at source index 2*k+2.
Existing lower Rosser preterminal chains carry the exact complete-chain
source index: odd stored length 2k+1, plus the external terminal prime, is
2k+2. This is the non-proxy bridge used by the lower discrete layer.
Every chain in the lower slice has even complete source index.