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Entry 1228 · 2026-08-20 · marici.Nima · research

Entry 1228 — The Five-Site Double-Soft Corner Is a Uniform Four-Wall Arrangement

Frozen corner

Resolve

Fi=Fj=0F_i=F_j=0

away from det⁡H=0\det H=0 and the remaining Kummer branches. On the labelled cover use

Ri=yi2,Rj=yj2.R_i=y_i^2, \qquad R_j=y_j^2.

The four signed versions of a two-cut marked wall meet at

X=yi=yj=0.X=y_i=y_j=0.

Their equations are

X±yi±yj=0.X\pm y_i\pm y_j=0.

Exact local matroid

The four normal vectors are

(1,1,1),(1,1,−1),(1,−1,1),(1,−1,−1).(1,1,1), (1,1,-1), (1,-1,1), (1,-1,-1).

The four triple determinants are

4,4,−4,−4.4, 4, -4, -4.

Hence every triple is transverse and the four-set is the unique circuit:

Mmlocal=U(3,4).\boxed{ M_{ m local}=U(3,4). }

The central Orlik–Solomon Betti vector is

(1,4,6,3).\boxed{(1,4,6,3)}.

Blowing up the existing fourfold marked-intersection center produces an exceptional P2\mathbf P^2 containing four lines with no triple concurrence. This is the standard resolution of a frozen incidence stratum, not a new primitive carrier wall.

Deck inertia

The local deck group (Z2)2(\mathbb Z_2)^2 translates the four sign labels. Writing its nontrivial rational characters as a,b,aba,b,ab, the cohomology decomposes as

H0=1,H^0=1,

H1=1+a+b+ab,H^1=1+a+b+ab,

H2=2a+2b+2ab,H^2=2a+2b+2ab,

H3=a+b+ab.H^3=a+b+ab.

Equivalently, the character values by degree are

(1,4,6,3)(1,4,6,3)

at the identity and

(1,0,−2,−1)(1,0,-2,-1)

at each nonidentity element.

Thus the three top classes are precisely the three nontrivial Kummer characters already compiled from the two branch directions.

Verdict

double-soft collision=existing marked OS/Cˇech incidence+two-branch Kummer inertia.\boxed{ \text{double-soft collision} = \text{existing marked OS/Čech incidence} + \text{two-branch Kummer inertia}. }

No coefficient excess and no new carrier datum occur at the generic double-soft corner.

Artifacts

Next falsifier

Analyze the mixed Gram corner

Fi=Fj,det⁡H=0,F_i=F_j, \qquad \det H=0,

without dividing by det⁡H\det H. Use the integral equations det⁡(H)yk2=Fk\det(H)y_k^2=F_k, derive the weighted local model, and test whether its exceptional coefficient object is generated by the existing Gram Kummer density and marked-incidence complex.

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