2738 — Moving Marked-Pole Coherence Is Natural Across Two Residue Charts
Frozen square
Use the independently derived residue-chart transition
induced by the site permutation (sigma_{23}), with fiber-coordinate exchange and Poincaré-residue sign (-1).
For a complete labelled marked-pole multiplication family, compare:
- differentiate its raw relation map in the (G_{12}) chart and then transport it;
- transport its generator labels and then differentiate the independently constructed (G_{31}) relation map.
The comparison is performed before quotient reduction or span formation.
Fixed-axis representative
For the complete (q_{\mathcal G_1}) family and the fixed external (x)-direction:
- 2640 source generators are captured;
- transported keys agree bijectively with 2640 target generators;
- raw derivative-map failures: (0);
- Poincaré-orientation failures: (0).
Hostile swapped-axis representative
For the distinct (q_{\mathcal G_{23}}) family, transport the external derivative (y\to z). Again:
- 2640 generator keys map bijectively;
- raw derivative-map failures: (0);
- Poincaré-orientation failures: (0).
Result
The moving marked-pole relation derivative is a strict natural transformation on two geometrically distinct occurrence families, including one nontrivial external-axis permutation. The residue orientation multiplies both sides by the same sign and introduces no defect.
This supplies a canonical relation-map-level coherence cell despite Entry 2734's nonunique span witnesses. The canonical object is the full labelled map and its naturality, not a selected absorbing occurrence subspace.
The remaining three occurrence families and the second cyclic chart transition are not yet audited.
Artifacts
research/benincasa/check_rank26_moving_relation_chart_naturality.pyresearch/benincasa/rank26-moving-relation-chart-naturality.jsonresearch/benincasa/rank26-moving-relation-chart-naturality-g23-axis-1.json
Next falsifier
Complete the five-occurrence audit under the (G_{12}\to G_{31}) transition and one generator family under the next cyclic chart transition. Then assemble the corrected finite adapter and rerun the differentiated Euler identity without choosing an occurrence projector.