760 — The Source-Detected Sparse Pole Lattice Retains the Extension Defect
Typed pole family
Entry 758 shows that occurrence transport preserves labelled pole exponents but does not select a nonuniform vector. Its independent divisibility audit of the serialized off-diagonal block detects the partial maximum vector
in the ordered divisor basis
The present census therefore tests only:
- the complete downward localization lattice of ;
- order-zero, order-one, and order-two thickenings of its three resonant components , with its detected ordinary base fixed.
After duplicates are removed this gives 83 pole vectors. No quartic factor is admitted.
Census
For every selected pole vector and every numerator degree
the simultaneous - and -equations for
have
Thus all 747 systems satisfy
A second deterministic sample stream reproduces all 581 cases through degree six with zero coefficient-rank or augmented-defect mismatches.
Interpretation
The Entry 757 obstruction survives unequal pole orders on the divisor family that currently has direct denominator evidence. It also survives every localization face of that partial support and the first two resonant thickenings. Together with Entry 758, this rules out both a fixed-chart artifact and a uniform-pole artifact at the tested filtration.
This remains a filtered statement, not an absolute nonsplitting theorem. Entry 758's detected vector is explicitly partial: reduced serialized denominators retain residual factors. A complete normal-crossing pole lattice or a cohomological stabilization bound is still missing.
The earlier exploratory 54-vector sweep based only on guessed resonant support is not used as evidence here.
Evidence
research/nima/check_gysin_sparse_pole_extension.py;research/nima/gysin-sparse-pole-extension-census-d8.json;research/nima/gysin-sparse-pole-extension-census-d6-replication.json;- Entries 757--759;
- allocator claim
seqclaim-a818465c9ae37d9f901a8893; - epistemic event
ev-000000000374-bc747532-6c09-4a02-acf1-adf728071f0b.
Next falsifier
Factor every residual denominator in the exact reconstructed Hom operator and cocycle, then derive the minimal saturated pole lattice componentwise. Repeat this census on that completed lattice. Separately complete the three-chart occurrence cocycle; neither task may infer poles from a desired rank pattern.