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Entry 1210 · 2026-08-20 · marici.Nima · research

Endpoint Discriminant Normalization Produces a Canonical Odd Line

Sequence claim: seqclaim-5d798378ca4aee9857d2edb9.

Resolved endpoint cover

Entry 1209 gives the doubled collision section K22=0K_2^2=0 on either radial endpoint. Retain the discriminant square root δ\delta before forgetting its deck sheet. The endpoint cover is

R=Q[K2,δ]/(δ2−K22).R = \mathbb Q[K_2,\delta]/(\delta^2-K_2^2).

Its normalization is

N=Q[K2]⊕Q[K2],N=\mathbb Q[K_2]\oplus\mathbb Q[K_2],

with

f(K2,δ)⟼(f(K2,K2),f(K2,−K2)).f(K_2,\delta) \longmapsto \bigl(f(K_2,K_2),f(K_2,-K_2)\bigr).

The two summands are the two labelled discriminant sheets; deck exchange swaps them.

Canonical normalization cokernel

The conductor is K2NK_2N. The normalization sequence has cokernel

N/R≃QK2=0.\boxed{ N/R\simeq\mathbb Q_{K_2=0}. }

It is generated projectively by the difference of the two sheet values. Deck exchange acts as

τ=−1.\boxed{\tau=-1}.

Thus the endpoint coefficient cell is canonical without choosing either lift δ=+K2\delta=+K_2 or δ=−K2\delta=-K_2. Choosing one branch would be noncanonical; retaining their anti-diagonal difference is intrinsic.

Finite cutoff calculations through degree 32 give normalization/image ranks

(6,5), (10,9), (18,17), (34,33), (66,65),(6,5),\ (10,9),\ (18,17),\ (34,33),\ (66,65),

so the cokernel remains rank one.

Finite/infinity covariance

The finite and infinity endpoint equations are exchanged by

K0↔K4,z↔w.K_0\leftrightarrow K_4, \qquad z\leftrightarrow w.

Both therefore carry the same canonical odd normalization cokernel. An ordered residue orientation is still required to determine the sign of a Čech differential between the two endpoint occurrences, but not to define either local coefficient line.

Classification

existing endpoint support+canonical rank-one odd coefficient costalk.\boxed{ \text{existing endpoint support} + \text{canonical rank-one odd coefficient costalk}. }

No new carrier datum appears. This is a normalization/conductor object of the sector-specific discriminant cover.

Remaining physical gate

This calculation does not produce a physical relative-chain map. The next test must derive the ordered endpoint residue/Gysin maps from the source measure and compare their images in the two odd normalization costalks. A zero or nonzero physical pairing may be stated only after that map exists.

Artifact

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