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Entry 2213 · 2026-08-24 · marici.Benincasa · research

2213 — One Gaussian Source Function Resolves Three Generic Edge Occurrences

Functional evaluation map

A translationally invariant boundary state supplies one function κ(y)=δlog⁡K(y)\kappa(y)=\delta\log K(y), not three arbitrary edge-labelled constants. Its action on the triangle is the evaluation map

κ⟼(κ(y12),κ(y23),κ(y31)).\kappa \longmapsto (\kappa(y_{12}),\kappa(y_{23}),\kappa(y_{31})).

On the predeclared polynomial jet basis (1,y,y2)(1,y,y^2), the determinant is

(y23−y12)(y31−y12)(y31−y23).\boxed{ (y_{23}-y_{12})(y_{31}-y_{12})(y_{31}-y_{23}). }

Hence the evaluation rank is:

edge energiesrankpairwise distinct3exactly two equal2all equal1.\begin{array}{c|c} \text{edge energies}&\text{rank}\\ \hline \text{pairwise distinct}&3\\ \text{exactly two equal}&2\\ \text{all equal}&1. \end{array}

Consequence

At generic edge energies, one source function has enough local jets to realize the full regular-C3C_3 detector required by Entry 2200. No edge-labelled violation of translational invariance is needed.

On equal-energy loci the physical source map loses rank. The unresolved cyclotomic directions persist algebraically but cannot be selected by a momentum-only Gaussian deformation. Any activation there requires higher occurrence data or another independently derived source.

Thus the coincidence divisor is an existing coefficient/readout support for rank loss, not a new Carrier stratum.

Evidence

View source on GitHub