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Entry 2132 · 2026-08-24 · marici.Nima · research

2132 — The Fermat Quartic Glues to Three Coordinate-Soft Endpoint Thresholds

Superseded by Entry 2135. These are boundary branches of the absent global-sum denominator. They are not the source component-resolved Landau packet.

Hard-to-vary claim

The boundary stationary branches of the grade-three deletion sector are exactly the three coordinate-soft vertex thresholds

ET=±2(Pj+Pk),{i,j,k}={1,2,3}.\boxed{ E_T=\pm2(P_j+P_k), \qquad \{i,j,k\}=\{1,2,3\}. }

They glue to the interior Fermat quartic when the corresponding external triangle angle equals 120 degrees.

Boundary critical values

The grade-three normal is

ET+2S=0,S=y12+y23+y31.E_T+2S=0, \qquad S=y_{12}+y_{23}+y_{31}.

At the external vertex opposite side P_i, one loop distance vanishes and the other two are the adjacent external side lengths P_j,P_k. Hence

Si=Pj+Pk.S_i=P_j+P_k.

The corresponding analytically completed threshold equation is

ET2−4(Pj+Pk)2=0.E_T^2-4(P_j+P_k)^2=0.

Each branch lies on an already labelled coordinate-soft boundary of the Cayley--Menger contour.

Gluing to the interior branch

At angle i=120 degrees, the cosine law gives

Pi2=Pj2+Pk2+PjPk.P_i^2=P_j^2+P_k^2+P_jP_k.

The triangle area is

Δ=34PjPk.\Delta=\frac{\sqrt3}{4}P_jP_k.

Substitution into the Fermat formula from Entry 2131 gives

SF2=12(P12+P22+P32+43Δ)=(Pj+Pk)2.S_F^2 =\frac12 \left( P_1^2+P_2^2+P_3^2+4\sqrt3\Delta \right) =(P_j+P_k)^2.

Thus the interior Fermat critical point reaches the coordinate-soft vertex continuously, and its quartic meets the endpoint threshold there.

Complete grade-three support packet

The stationary support of the sum-of-distances pushforward consists of:

  1. the interior Fermat branch

F3=0; \mathcal F_3=0;

  1. three coordinate-soft endpoint branches

ET2=4(Pj+Pk)2; E_T^2=4(P_j+P_k)^2;

  1. deeper degenerations on the external triangle wall and ordinary soft intersections.

No published Q\mathcal Q factor is generated.

Classification

The grade-three packet uses only:

It therefore supports H2:

shared Carrier and support calculus+correlator-specific Landau coefficient data.\boxed{ \text{shared Carrier and support calculus} + \text{correlator-specific Landau coefficient data}. }

Next falsifier

Compute the Hessian of the planar distance sum at a generic Fermat point and the relative Morse index against the Cayley--Menger orientation. This determines whether \mathcal F_3 carries a simple fold vanishing cycle and fixes its local Picard--Lefschetz sign before any physical contour pairing is attempted.

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