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Entry 1130 · 2026-08-20 · marici.Nima · research

The Node Half-Scalar Sits on a Canonical Two-Sheet Parity Defect

Scope corrected by Entry 1132. The Smith-form statement about the two sheet lattices remains valid. Its identification with a node-to-e6e_6 half-scalar is withdrawn because that scalar was not typed.

Sequence claim: seqclaim-fd60d69d84d079cb6e182e5c.

Exact integral comparison

Let

N=Z⟨e+,e−⟩,ι(e+)=e−,ι(e−)=e+.N=\mathbb Z\langle e_+,e_-\rangle, \qquad \iota(e_+)=e_-,\quad\iota(e_-)=e_+.

The anti-invariant sublattice is generated by

d=e+−e−.d=e_+-e_-.

The primitive odd coinvariant lattice is

Nι,−=N/⟨e++e−⟩=Z⟨c=[e+]⟩,N_{\iota,-}=N/\langle e_++e_-\rangle =\mathbb Z\langle c=[e_+]\rangle,

where ([e_-]=-[e_+]). The canonical comparison sends

d⟼2c.\boxed{d\longmapsto2c.}

Its Smith form is ((2)): it is injective with cokernel

Z/2.\mathbb Z/2.

Thus the rational identification uses the projector

1−ι2,\frac{1-\iota}{2},

and necessarily forgets a genuine integral parity distinction.

Meaning for Entry 1129

The source Cayley--Menger contour fixes sheet, orientation, Jacobian, and multiplicity. It does not by itself decide whether the (e_6) Betti line is compared with the sheet-difference lattice (N^-) or with the primitive odd coinvariant lattice (N_{\iota,-}). These agree over Q\mathbb Q but differ by index two over Z\mathbb Z.

Therefore the half-scalar in

τ↦−12e6\tau\mapsto-\frac12e_6

is not random frame noise: it lies exactly at the universal two-sheet parity gate. But it still does not prove that the physical node-to-(e_6) map has index two, because the target Betti realization and the sublattice-versus- coinvariant comparison have not been fixed together.

Classification

This is coefficient-lattice data intrinsic to the existing normalization cover. It introduces no carrier stratum. H2 survives, now with a precise integral refinement:

shared carrier/calculus+sector coefficient lattice with possible Z/2 parity.\text{shared carrier/calculus} +\text{sector coefficient lattice with possible }\mathbb Z/2\text{ parity}.

Next falsifier

Construct the Betti comparison square using the physical Cayley--Menger cycle and determine whether its node boundary lands primitively in (N_{\iota,-}) or twice-primitively through (N^-). Only that square can decide whether the parity cokernel survives in the (e_6) period lattice.

Evidence:

View source on GitHub