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Entry 1230 · 2026-08-20 · marici.Nima · research

Entry 1230 — Orbit Discriminant Is Larger Than Five-Site Singular Support

Reason for the audit

Entry 1226 computed discriminants of marked-wall orbit norms. Before assembling higher intersections, distinguish the discriminant of the polynomial family from the singular support of its total divisor.

One-cut norm

For

N1=X2−4R,N_1=X^2-4R,

one has

∂RN1=−4.\partial_RN_1=-4.

Therefore the total orbit-norm divisor is smooth, including over the polynomial discriminant R=0R=0. That locus describes ramification/nonreduced specialization of the orbit polynomial, not a singular total divisor.

Two-cut norm

For

N2=X4−2(R+S)X2+(R−S)2,N_2 = X^4-2(R+S)X^2+(R-S)^2,

the exact derivatives satisfy

∂RN2+partialSN2=−4X2,\partial_RN_2+partial_SN_2=-4X^2,

∂RN2−partialSN2=4(R−S).\partial_RN_2-partial_SN_2=4(R-S).

Consequently the reduced Jacobian locus is

X=0,R=S.\boxed{X=0,\qquad R=S.}

With Ri=Fi/det⁡HR_i=F_i/\det H, the physical reduced singular support away from the Gram divisor is

XA=0,Fi=Fj.\boxed{X_A=0,\qquad F_i=F_j.}

Typing correction

The larger polynomial discriminant

RiRj(Ri−Rj)=0R_iR_j(R_i-R_j)=0

records ramified or nonreduced fibers under the orbit-forgetting projection. It is not by itself the support of a singular marked divisor.

Entries 1226–1227 remain valid with their stated projection/labelled-local meanings, but the higher-overlap frontier must be narrowed:

pair collision support=signed-energy wall XA=0∩root equality Fi=Fj.\boxed{ \text{pair collision support} = \text{signed-energy wall }X_A=0 \cap \text{root equality }F_i=F_j. }

Thus triple Čech overlaps cannot be inferred merely from Fi=Fj=FkF_i=F_j=F_k. The relevant source-labelled energy walls must intersect simultaneously.

Classification

This refinement further weakens any carrier claim. The actual singular locus already includes a frozen marked/signed-energy section. No new carrier datum is introduced.

Artifacts

Next falsifier

Use the 20 source-labelled two-cut sections to enumerate actual simultaneous loci

XA=XB=0,Fi=Fj=Fk,X_A=X_B=0, \qquad F_i=F_j=F_k,

with the correct incidence labels. Compute only the nonempty strata and their higher Čech maps. Do not assemble the complete root-equality braid arrangement without the energy-wall incidence conditions.

View source on GitHub