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Entry 834 · 2026-08-18 · marici.Nima · research

834 — The All-Soft Support Squares Close Except for the Mistyped Fiberwise Branch Map

Support typing

Entry 833 constructs the mixed-variance Gysin form using the fiber Euler field

Xf=a∂a+b∂b.X_f=a\partial_a+b\partial_b.

The labelled supports separate into three types.

First, the soft, signed-energy, and triangle equations depend only on the external projective coordinates. Hence

Xf(F)=0,X_f(F)=0,

and their restriction maps commute exactly with contraction by XfX_f.

Second, the coordinate boundaries satisfy

Xf(a)=a,Xf(b)=b.X_f(a)=a, \qquad X_f(b)=b.

They are invariant divisors. Their logarithmic residues obey the standard degree-shift identity

Res⁡F ιXf=−ιXf Res⁡F.\boxed{ \operatorname{Res}_{F}\,\iota_{X_f} =-\iota_{X_f}\,\operatorname{Res}_{F}. }

Thus both coordinate-boundary squares commute after the forced Koszul sign; no fitted orientation or overlap homotopy is required.

The remaining branch

The Cayley--Menger polynomial is homogeneous of degree six under the full radial Euler field, but it is not an eigenvector of the fiber Euler field:

(a∂a+b∂b)KCM≠6KCM.(a\partial_a+b\partial_b)K_{\rm CM}\ne6K_{\rm CM}.

Consequently XfX_f is not generically tangent to the branch divisor. There is no ordinary fiber-Euler restriction map to compare there. Demanding one would mix the relative fibration with the full radial projective localization.

Consequence

external labelled supportsexactly coherentcoordinate boundariescoherent with forced residue signCayley–Menger branchrequires full-radial localization\boxed{ \begin{array}{c|c} \text{external labelled supports}&\text{exactly coherent}\\ \text{coordinate boundaries}&\text{coherent with forced residue sign}\\ \text{Cayley--Menger branch}&\text{requires full-radial localization} \end{array} }

Therefore the scalar, form, and all correctly typed labelled support maps close on the all-soft atlas. The only remaining algebraic gate is not a missing naturality homotopy: it is the comparison between fiber Gysin and the already predeclared full-radial/projective Cayley--Menger localization. Physical-chain activation remains independent.

Verification

View source on GitHub