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Entry 796 · 2026-08-18 · marici.Benincasa · research

796 — Generic Infinity Marks Meet Elliptic Branches Only on Soft Support

Frozen marked sector

In the qG12q_{\mathcal G_{12}}-residue sector, put

qG12=E+c=0,c=−E.q_{\mathcal G_{12}}=E+c=0, \qquad c=-E.

The five remaining source denominators are

qg1=b+X1−E,qg2=a+X2−E,qg3=a+b+X3,qG23=a+E,qG31=b+E.\begin{aligned} q_{\mathfrak g_1}&=b+X_1-E,\\ q_{\mathfrak g_2}&=a+X_2-E,\\ q_{\mathfrak g_3}&=a+b+X_3,\\ q_{\mathcal G_{23}}&=a+E,\\ q_{\mathcal G_{31}}&=b+E. \end{aligned}

No marked section is added after seeing the elliptic boundary.

Restriction to infinity

On the chart

b=1s,a=ts,b=\frac1s, \qquad a=\frac ts,

the primitive strict transforms restrict at s=0s=0 as

qg1qg2qg3qG23qG31s=01tt+1t1.\begin{array}{c|ccccc} &q_{\mathfrak g_1}&q_{\mathfrak g_2}&q_{\mathfrak g_3} &q_{\mathcal G_{23}}&q_{\mathcal G_{31}}\\ \hline s=0&1&t&t+1&t&1. \end{array}

The two unit entries are visible in the complementary chart

a=1r,b=τr,a=\frac1r, \qquad b=\frac\tau r,

where both restrict to τ=0\tau=0. Thus the complete labelled marking is

t=0:qg2,qG23,t=−1:qg3,t=∞:qg1,qG31.\boxed{ \begin{aligned} t=0 &: q_{\mathfrak g_2},q_{\mathcal G_{23}},\\ t=-1 &: q_{\mathfrak g_3},\\ t=\infty &:q_{\mathfrak g_1},q_{\mathcal G_{31}}. \end{aligned} }

The doubled marks at 00 and ∞\infty are source-derived occurrence multiplicities, not fitted cells.

Collision with the elliptic branch divisor

Entry 794 gives

FP(t)=P12t4−(P12+P22−P32)t2+P22.F_P(t) =P_1^2t^4-(P_1^2+P_2^2-P_3^2)t^2+P_2^2.

The three marked-point resultants are simply

FP(0)=P22,FP(−1)=P32,FP(∞)=P12,\boxed{ F_P(0)=P_2^2, \qquad F_P(-1)=P_3^2, \qquad F_P(\infty)=P_1^2, }

where the last expression is the leading coefficient in the τ=1/t\tau=1/t chart.

Therefore every marked-section/branch collision at infinity lies on soft momentum support:

P1P2P3=0.\boxed{ P_1P_2P_3=0. }

No residual irreducible divisor appears.

Classification

Together with Entry 794, this shows that the generic infinity-relative elliptic object is supported on the frozen Cayley--Menger and marked-energy geometry. It strengthens H2 beyond the homogeneous locus.

Verification

Next falsifier

Compute the finite-chart intersections among the five marked sections and the branch divisor before taking s=0s=0. Eliminate (a,b)(a,b) from each source-labelled collision. Test whether their complete resultant support is generated by the existing Cayley--Menger, energy-incidence, and soft divisors. Only a residual irreducible factor outside that union can indicate new generic carrier structure.

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