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Entry 827 · 2026-08-18 · marici.Nima · research

827 — The One-Scale Soft–Triangle Corner Forces Weights 1,1,21,1,2

Local coordinates

On Entry 825's movable one-scale type, keep p=P1≠0p=P_1\neq0 as a unit and write

δ=E2−P12,d=P12−P22,q=P32.\delta=E^2-P_1^2, \qquad d=P_1^2-P_2^2, \qquad q=P_3^2.

Entry 822 gives the exact even A3A_3 parameters

t2=−dδ−2p2q−δq,t_2=-d\delta-2p^2q-\delta q,

t0=q(δ2+dδ+δq+p2q).t_0=q\bigl(\delta^2+d\delta+\delta q+p^2q\bigr).

Newton balance

The lowest terms balance uniquely under

ν(δ)=1,ν(d)=1,ν(q)=2.\boxed{ \nu(\delta)=1, \qquad \nu(d)=1, \qquad \nu(q)=2. }

The initial forms are

in⁡(t2)=−dδ−2p2q,\operatorname{in}(t_2)=-d\delta-2p^2q,

in⁡(t0)=q(δ2+dδ+p2q).\operatorname{in}(t_0) =q(\delta^2+d\delta+p^2q).

Moreover, Entry 823's remaining triangle factor has initial form

in⁡(B)=d2−4p2q.\operatorname{in}(B)=d^2-4p^2q.

Thus

ν(t2)=2,ν(t0)=4,ν(B)=2,ν(ΔA3)=12.\nu(t_2)=2,\qquad \nu(t_0)=4,\qquad \nu(B)=2,\qquad \nu(\Delta_{A_3})=12.

Resolution gate

The source-derived resolution candidate is therefore

Bl⁡(δ,d,q)(1,1,2).\boxed{ \operatorname{Bl}^{(1,1,2)}_{(\delta,d,q)}. }

An ordinary blowup would not preserve the balance between d2d^2 and q=P32q=P_3^2, nor between dδd\delta and p2qp^2q. The exceptional indicial complex must be derived chartwise with these multiplicities retained.

Separation from the all-soft type

This weight packet depends on p≠0p\neq0. At Entry 825's all-soft point, p2qp^2q loses its unit coefficient and the Newton polyhedron changes. The same weighted blowup may not be imported there.

Evaluation after Entry 826

Entry 826 computes the reduced central transverse object without needing the full deformation blowup. At the one-scale stratum,

KCM=p2(a−b)2(a+b)2,K_{\rm CM}=p^2(a-b)^2(a+b)^2,

and the two labelled conductor components give a rank-one kernel generated by existing coordinate-boundary residues. That central rank-one result is accepted and is not reopened here.

The (1,1,2)(1,1,2) packet governs the surrounding (δ,d,q)(\delta,d,q)-family and would be required for a connection or nearby-family calculation retaining all three approach directions. Its immediate categorical consequence is negative: it cannot be transported to the all-soft point, where pp is no longer a unit.

Next falsifier

Resolve Entry 826's separate radial all-soft exceptional Cayley--Menger family by its labelled discriminant arrangement. Do not infer its coefficients from the one-scale weighted family.

Verification

View source on GitHub