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Entry 813 · 2026-08-18 · marici.Benincasa · research

813 — Coordinate-Boundary Sextics Develop an A3 Soft-Signed Excess

Frozen object

Use Entry 807's source-normalized Cayley--Menger polynomial in

A=a2,B=b2A=a^2,\qquad B=b^2

and retain the ordered residue orientation da∧dbda\wedge db. This entry analyzes the labelled coordinate boundaries; it does not infer multiplicity from the scalar sextic.

The single a=0a=0 branch

On P2≠0P_2\ne0, complete the BB-square and call the translated coordinate yy. The exact formal expression is

KCM=P22y2+Λ4P22[4E2P22−(a2−(E2+P22))2].\boxed{ K_{\rm CM} =P_2^2y^2+ \frac{\Lambda}{4P_2^2} \left[4E^2P_2^2-\bigl(a^2-(E^2+P_2^2)\bigr)^2\right]. }

Consequently the branch discriminant is

−(E−P2)2(E+P2)2Λ4P22.-\frac{(E-P_2)^2(E+P_2)^2\Lambda}{4P_2^2}.

At a generic signed-energy point E=±P2E=\pm P_2, with Λ≠0\Lambda\ne0, the completed fiber is an A1A_1 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 A1A_1 monodromy; the resolved occurrence remembers the sheet.

At generic Λ=0\Lambda=0, the aa-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 E=±P2E=\pm P_2 together with Λ=0\Lambda=0, the reduced signed and triangle divisors meet regularly. Their iterated vanishing rank remains one, with no reduced excess Tor⁡1\operatorname{Tor}_1; the signed direction retains its length-two Cartier layer.

The locus E=0E=0 is not a singular branch here at generic P2Λ≠0P_2\Lambda\ne0. When P2=0P_2=0, the affine critical section BcritB_{\rm crit} has a pole and exits to the infinity/soft closure. It must not be counted as another finite a=0a=0 class.

The labelled b=0b=0 branch

The source-labelled exchange

(a,P2)⟷(b,P1)(a,P_2)\longleftrightarrow(b,P_1)

gives the second completion. Its support is

E−P1=0,E+P1=0,Λ=0,E-P_1=0,\qquad E+P_1=0,\qquad \Lambda=0,

with the same A1A_1, 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 a=b=0a=b=0,

KCM=P32R00,K_{\rm CM}=P_3^2R_{00},

where

R00=E4−E2(P12+P22−P32)+P12P22.R_{00}=E^4-E^2(P_1^2+P_2^2-P_3^2)+P_1^2P_2^2.

At a generic point of either P3=0P_3=0 or R00=0R_{00}=0, the two quadratic normal coefficients do not vanish simultaneously. The local singularity is A1A_1, generated respectively by the existing soft nearby cycle or the restricted Cayley--Menger Gysin map. The soft normal enters through P32P_3^2, hence carries a length-two Cartier layer.

There is a genuine enhancement at the soft--signed corners

P3=0,E2=P12orP3=0,E2=P22.P_3=0,\quad E^2=P_1^2 \qquad\text{or}\qquad P_3=0,\quad E^2=P_2^2.

After the appropriate labelled exchange and absorption of units, the completed fiber is

w2+b2+a4=0.\boxed{w^2+b^2+a^4=0.}

This is A3A_3, with Jacobian algebra

k[[a]]/(a3)k[[a]]/(a^3)

and therefore

μ=3.\boxed{\mu=3.}

All three vanishing cycles are anti-invariant under the cover involution. The intrinsic A3A_3 monodromy eigenvalues are i,−1,−ii,-1,-i. 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

rank⁡phisoft,signed=3versus generic Kato rank 1.\boxed{ \operatorname{rank}phi_{\rm soft,signed}=3 \quad\text{versus generic Kato rank }1. }

This is coefficient complexity on an existing labelled carrier intersection, not evidence for a new carrier divisor.

When additionally P12=P22P_1^2=P_2^2, equivalently on the deeper soft--triangle corner, the A3A_3 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 A3A_3 extension on the existing intersection without adding a carrier cell.

Verification

Next falsifier

Construct the iterated soft--signed nearby-cycle complex at one labelled A3A_3 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.

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