The Two-Cut Koszul Determinant Is Not Source Realized
Question
Entry 361 excluded ordinary nearby cycles and the ordinary Euler class as sources of the missing overlap retraction. The remaining source-native candidate was the ordered two-normal Koszul determinant. The hard-to-vary claim tested here is
No joint pole, product of source summands, secondary kernel, or support cell is inserted.
Completed normal grammar
Put
On the generic common open, all lower denominators and the Cayley--Menger coefficient are units in the completed normal ring. Their Taylor expansions contain only nonnegative powers of (u,v). The frozen physical source is therefore locally of the form
with (A,B,C\in R[[u,v]]). Its negative Laurent support is contained in
Top Cousin projection
For the regular sequence ((u,v)), the top local-cohomology quotient is
Only Laurent monomials negative in both variables survive. The primitive ordered determinant class is represented by
with support ((-1,-1)).
Both singly polar source terms map to zero in this quotient. Addition and the linear Cousin differential do not multiply them. Hence
The geometric Koszul determinant exists, but the frozen physical coefficient form does not realize it.
Verdict
The tested claim is falsified. Producing the determinant requires either
or an independently derived secondary correspondence kernel with the same top Cousin grade. The first changes the source pole grammar; the second has not been derived. Neither is admissible as a repair.
Combined with Entries 357--361, this closes the frozen pairwise descent attack:
Classification
| Datum | Classification |
|---|---|
| regular sequence ((u,v)) | existing carrier normal geometry |
| ((uv)^{-1}) | geometric top Koszul/Cousin class |
| singly polar source support | sector-specific coefficient form |
| top Cousin projection | zero |
| missing determinant coefficient | absent secondary coefficient datum |
| new carrier stratum | none |
Consequence for the cosmology architecture
This does not falsify H2. H2 permits sector-specific coefficient objects and does not require their physical summands to satisfy Čech descent. It does falsify the stronger proposal that the three marked-Cut rank-twelve modules are glued by pairwise overlap transitions already present in the frozen six-term integrand.
The positive global structure should therefore be sought in the Cousin degree where the source actually lives: a cyclic sum of singly supported classes on the union of the three marked-Cut divisors, with zero pairwise top residue—not as a degree-zero sheaf assembled by overlap isomorphisms.
Evidence
research/benincasa/marici-gm/src/bin/two_cut_cousin_determinant_gate.rs;research/benincasa/two-cut-cousin-determinant-gate-certificate.json;- Entries 229 and 357--361.
Next falsifier
Construct the full three-divisor Cousin complex for
using the six frozen source occurrences. Place each singly marked summand in Cousin degree one, retain its lower-denominator occurrence label, and compute the differential to all three pairwise intersections and the triple intersection.
Test whether the all-positive cyclic source is a canonical nonzero degree-one cocycle with vanishing higher residues. If so, this identifies its global home without inventing transition maps. If it is exact or develops a nonzero higher residue after the full lower-boundary data are retained, the equivariant direct-sum interpretation must be revised.