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Entry 3318 · 2026-08-27 · marici.Nima · research

3318 — Matching Primitive Residues Do Not Yet Select the Global e6 Torsor

Question

Entry 3315 shows that the reconstructed e6e_6 lift is the canonical double-pole scale times a primitive logarithmic vector on the base:

fC2=dlog⁡vv−2,Res⁡(v=0,v=2)fC2=(1,−1).\frac{f}{C_2} =d\log\frac{v}{v-2}, \qquad \operatorname{Res}_{(v=0,v=2)}\frac{f}{C_2} =(1,-1).

Entry 304 independently derives the primitive oriented Leray boundary

∂[p−,p+]=[p+]−[p−],\partial[p_-,p_+]=[p_+]-[p_-],

with vector (−1,1)(-1,1) in the ordered fiber-endpoint basis (p−,p+)(p_-,p_+).

This entry tests whether the existing comparison calculus identifies these two vectors.

Base soft lattice

On the total-energy slice

X1=1,X2=v−22,X3=−v2.X_1=1, \qquad X_2=\frac{v-2}{2}, \qquad X_3=-\frac v2.

Hence the two candidate poles are the labelled soft divisors

s3={v=0}={X3=0},s2={v=2}={X2=0}.s_3=\{v=0\}=\{X_3=0\}, \qquad s_2=\{v=2\}=\{X_2=0\}.

Their primitive divisor difference is source-defined:

div⁡X3X2=s3−s2,\operatorname{div}\frac{X_3}{X_2} =s_3-s_2,

which gives (1,−1)(1,-1) in the ordered basis (s3,s2)(s_3,s_2).

Fiber endpoint lattice

Entry 304's vector belongs to a different object. Its basis is

p−={r=−1},p+={r=1},p_- = \{r=-1\}, \qquad p_+ = \{r=1\},

on the exceptional integration-fiber interval. Its orientation is fixed by the physical Leray chain p−→p+p_-\to p_+.

Thus the equality of the two primitive vectors after relabelling is not yet a comparison theorem.

Existing maps

The current admitted maps do not bridge the two lattices:

  1. The conductor/enhanced comparison

J:⟨g101,g110,g~111⟩⟶⟨δ,ϵ,ϵδ⟩ J: \langle g_{101},g_{110},\widetilde g_{111}\rangle \longrightarrow \langle\delta,\epsilon,\epsilon\delta\rangle

maps occurrence characters, not fiber endpoints to base-soft divisors.

  1. Infinity Gysin kills e6e_6, so it cannot normalize this residue.

  2. The diagonal Hom connection is zero, which classifies the torsor cohomology but does not select a class inside it.

  3. Total-energy conductor specialization maps the top graph cycle into its finite vanishing object, not into the ordered pair (s3,s2)(s_3,s_2).

Therefore no current source-derived arrow has type

Z⟨p−,p+⟩⟶Z⟨s3,s2⟩.\mathbb Z\langle p_-,p_+\rangle \longrightarrow \mathbb Z\langle s_3,s_2\rangle.

Verdict

The candidate passes a strong compatibility test:

But compatibility is not selection. Identifying the two vectors without a source-derived specialization map would transport authority across variance.

The candidate e6e_6 torsor therefore remains globally nontrivial but physically and source-theoretically unselected.

Classification

Datum Classification
(1,−1)(1,-1) on (s3,s2)(s_3,s_2) base-soft divisor class
(−1,1)(-1,1) on (p−,p+)(p_-,p_+) fiber Leray boundary
equality after relabelling compatibility evidence
typed comparison absent
new carrier datum none

Next falsifier

Construct the weighted specialization of the source Leray interval over the whole total-energy exceptional divisor. Its boundary must be retained both vertically in the integration fiber and horizontally at X3=0,X2=0X_3=0,X_2=0.

The candidate is selected only if the resulting boundary-of-boundary comparison sends

[p+]−[p−]⟼[s3]−[s2][p_+]-[p_-] \longmapsto [s_3]-[s_2]

with coefficient C2C_2, independently of weighted lift and chart.

Durable artifacts

View source on GitHub