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Entry 712 · 2026-08-18 · marici.Benincasa · research

712 — The Oriented Triple Incidence Does Not Lift the Signed Pair Relation

Frozen incidence calculation

Use the disappearing triple

(qg2,qg3,qg23)(q_{\mathfrak g_2},q_{\mathfrak g_3},q_{\mathfrak g_{23}})

and pair order

([23],[2,23],[3,23]).([23],[2,23],[3,23]).

Taking each ordered double residue and then the remaining residue gives

(r23,r2,23,r3,23)=(12,−12,12).\boxed{ (r_{23},r_{2,23},r_{3,23}) =\left(\frac12,-\frac12,\frac12\right).}

All three remaining linear forms vanish at the same triple point c=−X2c=-X_2. Hence the primitive oriented incidence vector is

(1,−1,1).\boxed{(1,-1,1).}

Failure of the proposed lift

Entry 709 proves the strict residue identity

[2,23]=[3,23].[2,23]=[3,23].

Their two contributions to the triple incidence therefore cancel, leaving the minus pair [23][23]. Applying Entry 707's branch-discriminant symbol gives

σ2(Disc⁡)(1,−1,1)=C23−ν2ν3,\sigma_2(\operatorname{Disc})(1,-1,1) =C_{23}^-\nu_2\nu_3,

which is generically nonzero. Consequently

the disappearing triple incidence is not a lift of the weighted signed-pair kernel relation.\boxed{ \text{the disappearing triple incidence is not a lift of the weighted signed-pair kernel relation}.}

This is a source-derived orientation test, not a rank argument.

What survives

Entry 711 gives the triple's first nonzero normal coefficient

T2=X32ν22+(X12−X22−X32)ν2ν3+X22ν32.T_2=X_3^2\nu_2^2 +(X_1^2-X_2^2-X_3^2)\nu_2\nu_3 +X_2^2\nu_3^2.

Thus the second-Rees triple costalk naturally lives on

η2=T2.\boxed{\eta^2=T_2.}

The mixed triple remains a valid Kummer coefficient object over the existing normal carrier, but it does not provide the sought polynomial chain homotopy between the signed pair residues.

Classification

No new carrier stratum is indicated.

Evidence

Next falsifier

Retire the direct triple-homotopy route. The remaining typed possibility is a nontrivial extension between the pair Kummer systems and the mixed triple costalk. Construct its Gauss--Manin connecting morphism on the quadratic normal cover and test whether its extension coefficient has Q\mathcal Q support. If no source-derived connecting morphism exists, this entire lower normal branch remains disconnected from the homogeneous Q\mathcal Q sector.

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