pith. sign in
theorem

doubledZeroDefect_recurrence

proved
show as:
module
IndisputableMonolith.NumberTheory.ZeroDoublingLaw
domain
NumberTheory
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plain-language theorem explainer

The doubling recurrence equates the doubled zero defect at complex ρ to twice the square of the zero defect plus four times the zero defect. Researchers examining the functional-equation and RCL bridge in Recognition Science cite it as the concrete Phase-4 self-composition law on the defect observable. The proof is a short algebraic reduction that substitutes the cosh closed forms, applies the double-angle identity, and closes via nlinarith on the cosh-squared relation.

Claim. Let $D(ρ)$ denote the zero defect and $D^{(2)}(ρ)$ the doubled zero defect at $ρ ∈ ℂ$. Then $D^{(2)}(ρ) = 2 [D(ρ)]^2 + 4 D(ρ)$.

background

The Zero Doubling Law module records the strongest concrete Vector C instantiation obtained from the functional-equation/J-symmetry bridge. The defect observable satisfies the doubling recurrence $D(2t) = 2 D(t)^2 + 4 D(t)$. The defect functional is defined as defect(x) := J(x) for positive x, where J is the Recognition Science cost J(x) = (x + x^{-1})/2 - 1. The doubled zero defect is constructed by applying the J-log functional to twice the zero deviation.

proof idea

The proof is a short tactic sequence. It rewrites both sides via the closed forms doubledZeroDefect_eq_cosh_sub_one and zeroDefect_eq_cosh_sub_one. It then invokes Real.cosh_two_mul for the double-angle formula on cosh. The step closes with nlinarith applied to the identity Real.cosh_sq (zeroDeviation ρ).

why it matters

This supplies the recurrence packaged into current_vectorC_attempt_data, which asserts the zero-defect equivalence to the critical line together with nonnegativity and the doubling law. It is also invoked inside pureVectorCDoublingData_of_zero to equip any completed-ξ zero with the pairing invariants plus the FE/RCL doubling recurrence. The result instantiates the Phase-4 self-composition law from the FE/RCL bridge, giving concrete evidence of nontrivial interaction between FE symmetry and the RS defect while remaining short of the full d'Alembert interface.

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