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Entry 838 · 2026-08-18 · marici.Benincasa · research

838 — The Generic All-Soft Polar Discriminant Splits into Two Labelled Fold Components

Question after Entries 836–837

Entry 837 canonically types the polar coefficient as

Ppol=ϕπ(KCM)\mathcal P_{\rm pol}=\phi_\pi(\mathcal K_{\rm CM})

and proves generic rank one from square-freeness. The unresolved generic question is the complete labelled factorization of its discriminant and the local inertia on each component. Triangle-wall specialization is not computed here.

Exact factorization

Along a fiber-scaling orbit, with z=s2z=s^2,

K(z)=K0+zK2+z2K4.K(z)=K_0+zK_2+z^2K_4.

Exact expansion over Z\mathbb Z gives

K22−4K0K4=Λ(P1,P2,P3)Q+Q−.\boxed{ K_2^2-4K_0K_4 = \Lambda(P_1,P_2,P_3)Q_+Q_-. }

Here

Λ=(P1−P2−P3)(P1−P2+P3)⋅(P1+P2−P3)(P1+P2+P3)\Lambda = (P_1-P_2-P_3)(P_1-P_2+P_3) \mathbin{\cdot}(P_1+P_2-P_3)(P_1+P_2+P_3)

and

Q±=E2(a2−b2)−P12a2+P22b2±2EP3ab.\boxed{ Q_\pm = E^2(a^2-b^2)-P_1^2a^2+P_2^2b^2 \pm2EP_3ab. }

Thus, away from Λ=0\Lambda=0, the polar discriminant is not an unlabelled binary quadratic. It consists of two conjugate occurrence components Q+=0Q_+=0 and Q−=0Q_-=0.

Their difference is

Q+−Q−=4EP3ab.Q_+-Q_-=4EP_3ab.

Consequently

V(Q+,Q−)⊂V(E)∪V(P3)∪V(a)∪V(b).\boxed{ V(Q_+,Q_-) \subset V(E)\cup V(P_3)\cup V(a)\cup V(b). }

The two generic components are disjoint away from already frozen total energy, soft, and coordinate-boundary support.

Generic local rank

On Q+=0Q_+=0, the rational point

(E,P1,P2,P3,a,b)=(−4,1,3,1,1,1)(E,P_1,P_2,P_3,a,b)=(-4,1,3,1,1,1)

satisfies

Λ=45,Q−=16,∂EQ+=2.\Lambda=45,\qquad Q_-=16,\qquad \partial_EQ_+=2.

Hence Q+Q_+ is a reduced transverse discriminant component there. The sign-reflected witness gives the same result for Q−Q_-. At a generic point of either component, with K4≠0K_4\ne0, completing the square gives

K(z)=K4ξ2−τ,K(z)=K_4\xi^2-\tau,

and the double cover has local form

W2=ξ2−τ.\boxed{W^2=\xi^2-\tau.}

Therefore each labelled component carries one relative fold class:

rank⁡Q±Ppol=1.\boxed{ \operatorname{rank}_{Q_\pm}\mathcal P_{\rm pol}=1. }

Two distinct inertia statements

The roots of the orbit quadratic are exchanged around Q±=0Q_\pm=0, so their reduced degree-zero permutation line has character −1-1. The vanishing generator of the complex-curve A1A_1 model W2=ξ2−τW^2=\xi^2-\tau, however, is fixed by its Picard–Lefschetz monodromy:

χroots=−1,Tvan=+1.\boxed{ \chi_{\rm roots}=-1, \qquad T_{\rm van}=+1. }

These must not be conflated. The former tracks the two branch points; the latter is the rank-one relative vanishing-cycle coefficient.

Classification

The factor Λ\Lambda is the existing momentum-triangle wall. The factors Q±Q_\pm are labelled coefficient-polar support internal to the source-defined projection. Their mutual collision occurs only on existing support. Hence

existing carrier+two rank-one labelled polar coefficient components\boxed{ \text{existing carrier} + \text{two rank-one labelled polar coefficient components} }

with no new carrier divisor inferred.

Verification

Join point

The next operation is the already typed specialization

ψΛϕπ(KCM).\psi_\Lambda\phi_\pi(\mathcal K_{\rm CM}).

It must determine how the two labelled fold lines meet the triangle Gysin object. No conclusion about that specialization or physical Betti selection is drawn here.

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