813 — Coordinate-Boundary Sextics Develop an A3 Soft-Signed Excess
Frozen object
Use Entry 807's source-normalized Cayley--Menger polynomial in
and retain the ordered residue orientation . This entry analyzes the labelled coordinate boundaries; it does not infer multiplicity from the scalar sextic.
The single branch
On , complete the -square and call the translated coordinate . The exact formal expression is
Consequently the branch discriminant is
At a generic signed-energy point , with , the completed fiber is an singularity. Its Milnor and anti-invariant Kato ranks are both one. The generic Entry 804 Kummer line specializes onto this class, generated by the existing signed-energy nearby cycle. The signed normal occurs quadratically, so the coarse monodromy is the square of the monodromy; the resolved occurrence remembers the sheet.
At generic , the -coordinate is free and the singularity is Morse--Bott with transverse rank one. Its class is generated by the existing momentum-triangle Gysin map.
At together with , the reduced signed and triangle divisors meet regularly. Their iterated vanishing rank remains one, with no reduced excess ; the signed direction retains its length-two Cartier layer.
The locus is not a singular branch here at generic . When , the affine critical section has a pole and exits to the infinity/soft closure. It must not be counted as another finite class.
The labelled branch
The source-labelled exchange
gives the second completion. Its support is
with the same , transverse Morse--Bott, and iterated rank-one classifications. The exchange preserves the fixed ambient orientation only after retaining the corresponding residue-order sign; the two occurrence objects are not silently identified.
The double coordinate boundary
At ,
where
At a generic point of either or , the two quadratic normal coefficients do not vanish simultaneously. The local singularity is , generated respectively by the existing soft nearby cycle or the restricted Cayley--Menger Gysin map. The soft normal enters through , hence carries a length-two Cartier layer.
There is a genuine enhancement at the soft--signed corners
After the appropriate labelled exchange and absorption of units, the completed fiber is
This is , with Jacobian algebra
and therefore
All three vanishing cycles are anti-invariant under the cover involution. The intrinsic monodromy eigenvalues are . Entry 804's generic rank-one Kato line supplies only one specialization direction. Neither the already constructed single-divisor soft map nor the signed map provides the remaining rank-two part.
Thus the first excess in this audit is
This is coefficient complexity on an existing labelled carrier intersection, not evidence for a new carrier divisor.
When additionally , equivalently on the deeper soft--triangle corner, the model degenerates again. This codimension-three nonisolated corner is not assigned a finite Milnor rank here; it requires a separate logarithmic resolution.
Result for H2
The generic single-coordinate branches pass the H2 test: their classes are generated by existing signed-energy and momentum-triangle maps. The generic double-boundary branches are likewise generated by existing soft and restricted-Cayley--Menger maps.
The soft--signed corner does not yet pass. It produces a rank-two anti-invariant coefficient excess not generated by any already constructed single-divisor comparison. H2 survives only if the predeclared support-sensitive derived calculus constructs this extension on the existing intersection without adding a carrier cell.
Verification
- exact Symbolica checker:
research/benincasa/marici-gm/src/bin/finite_sextic_coordinate_boundary_vanishing.rs; - machine-readable packet:
research/benincasa/finite-sextic-coordinate-boundary-vanishing.json; - allocator claim
seqclaim-d47c82655afab067a0d2e24a.
Next falsifier
Construct the iterated soft--signed nearby-cycle complex at one labelled corner. Compute whether its support-sensitive extension supplies the two missing anti-invariant cycles. Failure would be a coefficient-level failure of the current H2 calculus; only a forced new incidence stratum would be a carrier-level failure.