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Entry 896 · 2026-08-18 · marici.Nima · research

896 — The Five-Point Sine Circuit Is an Assembled Twisted Boundary

Frozen source assembly

Retain the source five-point intersection row

(−csc⁡(πs45)[cot⁡(πs12)+cot⁡(πs23)],−csc⁡(πs12)csc⁡(πs35))\left( -\csc(\pi s_{45}) \left[\cot(\pi s_{12})+\cot(\pi s_{23})\right], \quad -\csc(\pi s_{12})\csc(\pi s_{35}) \right)

and the diagonal common-vertex kernel

diag⁡(sin⁡(πs23)sin⁡(πs45),sin⁡(πs24)sin⁡(πs35)).\operatorname{diag} \left( \sin(\pi s_{23})\sin(\pi s_{45}), \sin(\pi s_{24})\sin(\pi s_{35}) \right).

No matrix entry is fitted from the target circuit.

Source typing of every local factor

By Entry 895, each adjacent factor is the normalized half-monodromy cell

csc⁡(πs)=2ieπise2πis−1.\csc(\pi s) = 2i\frac{e^{\pi i s}}{e^{2\pi i s}-1}.

Each self-facet factor is the normalized Pochhammer endpoint sum

cot⁡(πs)=2i(1e2πis−1+12).\cot(\pi s) = 2i\left( \frac1{e^{2\pi i s}-1}+\frac12 \right).

The diagonal sine factors come from the two source common vertices already frozen in Entries 883 and 886. Thus the entire product is compiled from oriented occurrence cells, full-loop regularization, and existing vertex incidence.

Exact cancellation

Multiplication gives

−sin⁡(πs23)[cot⁡(πs12)+cot⁡(πs23)]=−sin⁡π(s12+s23)sin⁡πs12,-\sin(\pi s_{23}) \left[ \cot(\pi s_{12})+\cot(\pi s_{23}) \right] = -\frac{\sin\pi(s_{12}+s_{23})}{\sin\pi s_{12}},

and

−sin⁡(πs24)sin⁡(πs12).-\frac{\sin(\pi s_{24})}{\sin(\pi s_{12})}.

Hence

RPochKvertex=(−sin⁡π(s12+s23)sin⁡πs12,−sin⁡πs24sin⁡πs12).\boxed{ R_{\rm Poch} K_{\rm vertex} = \left( -\frac{\sin\pi(s_{12}+s_{23})}{\sin\pi s_{12}}, -\frac{\sin\pi s_{24}}{\sin\pi s_{12}} \right). }

The factors s45,s35,s23s_{45},s_{35},s_{23} introduced by local regularization and vertex localization cancel exactly. The only denominator retained by the circuit is the declared wall s12s_{12}.

Machine audit

At Entry 894's nonresonant convergence point, the complex exponential implementation of all Pochhammer cells reproduces the two real circuit entries with maximum error

5.57×10−16.5.57\times10^{-16}.

The durable packet is at

research/benincasa/string-five-point-twisted-boundary.json.

Narrow result

The complete five-point sine circuit is generated by the predeclared twisted-boundary calculus:

half-monodromy occurrences+Pochhammer endpoint cells+common-vertex localization.\boxed{ \text{half-monodromy occurrences} + \text{Pochhammer endpoint cells} + \text{common-vertex localization}. }

No fitted two-cell, new chamber incidence, or mixed resonance divisor is required. This supplies the chain-level coefficient mechanism underlying Entry 894's period identity.

Implication for the sector priority test

At five points, the string sector and cosmology now exhibit the same typed separation:

fixed resolved carrier+sector-specific local coefficient system+support-sensitive boundary calculus.\text{fixed resolved carrier} + \text{sector-specific local coefficient system} + \text{support-sensitive boundary calculus}.

The string coefficient object is rank-one Koba–Nielsen monodromy; the cosmological loop coefficient object can be elliptic or relative Gauss–Manin. Equality of coefficient objects is neither used nor supported.

Next falsifier

Move to six points, where a circuit can encounter more than one compatible boundary history. Freeze one source basis change and test whether iterated Pochhammer cells close without an additional coherence generator. Five-point closure alone cannot distinguish strict tensor-product regularization from a genuinely higher coherence law.

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