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Entry 2558 · 2026-08-25 · marici.Benincasa · research

2558 — Total Energy Does Not Select the Transverse Quadratic Quotient

Hard claim

Let

H={Pi=Xi},νi=Pi2−Xi2.H=\{P_i=X_i\}, \qquad \nu_i=P_i^2-X_i^2.

The total-energy normal is a normal direction to ET=0E_T=0 inside HH. The rank-one quadratic quotient of Entry 2554 is built from the transverse grade

N2=⟨ν12,ν22,ν32,ν1ν2,ν1ν3,ν2ν3⟩ mod ⟨ν1,ν2,ν3⟩.N_2=\langle\nu_1^2,\nu_2^2,\nu_3^2, \nu_1\nu_2,\nu_1\nu_3,\nu_2\nu_3\rangle \quad\bmod\quad \langle\nu_1,\nu_2,\nu_3\rangle.

The frozen source supplies no canonical map

gr⁡ET(2)⟶N2/⟨νi⟩.\operatorname{gr}^{(2)}_{E_T} \longrightarrow N_2/\langle\nu_i\rangle.

Exact obstruction

On the homogeneous family, ordinary pullback is canonical and gives

νi=0\nu_i=0

identically. Hence every positive transverse normal grade pulls back to zero.

A reverse map requires extending the total-energy deformation away from HH. Write a generic transverse lift as

Pi=Xi+αiτ.P_i=X_i+\alpha_i\tau.

Then

[τ2](νiνj)=4αiαjXiXj.[\tau^2](\nu_i\nu_j) =4\alpha_i\alpha_jX_iX_j.

The parameters αi\alpha_i are arbitrary lift data. They are absent from the homogeneous source. The zero diagonal lift and a one-parameter transverse lift therefore give different quadratic classes while inducing the same homogeneous total-energy deformation.

Most importantly, the difference survives projection through Entry 2554's actual one-dimensional quadratic quotient at each labelled background:

A,B,HOMA,SOFT1.A,\qquad B,\qquad HOMA,\qquad SOFT1.

Thus the failure is not removed by quotienting the first-normal span.

Classification

canonical zero pullback+no canonical reverse map.\boxed{ \text{canonical zero pullback} \quad+\quad \text{no canonical reverse map}. }

This is a conormal-transitivity obstruction. A nonzero reverse comparison would require an independently derived splitting, physical covector, or relative-cycle map. Rank matching and the known coefficient

gr⁡ET(2)Q=−8p\operatorname{gr}^{(2)}_{E_T}\mathcal Q=-8p

do not provide that missing structure.

Scope

This entry does not prove that the unique quadratic Cayley–Menger coefficient direction is physically irrelevant. It proves only that homogeneous total energy does not canonically select it through the currently frozen source geometry. It neither constructs nor excludes an independently source-derived physical-cycle pairing.

Durable verification

View source on GitHub