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Entry 2461 · 2026-08-25 · marici.Benincasa · research

2461 — The Fixed Loop-Vector Cycle Faithfully Reads the Complete Interaction Score Tower

Question

Entry 2460 proves local score independence after moving the Cayley--Menger boundary in distance coordinates. Does this survive on the actual source cycle, without gradient pivots or Čech representatives?

Sequence claim: seqclaim-68bf7edede6ae644d31884e1.

Return to the primary cycle

In the original loop-vector representation the physical cycle is fixed:

Γℓ=R3.\Gamma_\ell=\mathbb R^3.

The Cayley--Menger square-root measure is the Jacobian of the change to loop distances. Before that change, the regulated four-wall density is simply

ρ(ℓ;ν)=1qg1qg2qg3qg23.\rho(\ell;\nu) = \frac1{ q_{g_1}q_{g_2}q_{g_3}q_{g_{23}} }.

Choose external vertices

v2=0,v3=(P2,0,0),v_2=0, \qquad v_3=(P_2,0,0),

v4=(P12+P22−P322P2,P12−(P12+P22−P322P2)2,0),v_4= \left( \frac{P_1^2+P_2^2-P_3^2}{2P_2}, \sqrt{P_1^2-\left( \frac{P_1^2+P_2^2-P_3^2}{2P_2} \right)^2},0 \right),

with

Pi2=Xi2+νi.P_i^2=X_i^2+\nu_i.

Then (c=|\ell-v_2|), (a=|\ell-v_3|), and (b=|\ell-v_4|) reproduce the source-labelled walls exactly.

Exact finite-field automatic differentiation

The checker expands the physical density in

Fp[ν1,ν2,ν3]/(ν)4\mathbb F_p[\nu_1,\nu_2,\nu_3]/(\nu)^4

and extracts the ten normalized responses labelled by

νi,quadνi2,quadνiνj,quadν1ν2ν3.\nu_i,quad \nu_i^2,quad \nu_i\nu_j,quad \nu_1\nu_2\nu_3.

Square roots are expanded inside the same truncated algebra. No distance-space gradient lift, fitted primitive, or numerical derivative is used.

At twenty-eight accepted loop points in each run, the exact ranks are

p(X1,X2,X3)rank⁡(R)rank⁡(1,R)32003(3,4,5)101132009(4,13,15)1011.\begin{array}{c|c|c|c} p&(X_1,X_2,X_3)&\operatorname{rank}(R)& \operatorname{rank}(1,R)\\ \hline 32003&(3,4,5)&10&11\\ 32009&(4,13,15)&10&11. \end{array}

A nonzero determinant modulo either good prime proves that the corresponding function-field determinant is not identically zero in characteristic zero. The independent replication excludes a single-prime or single-triangle accident.

Regulated physical consequence

On the positive real chamber the ten response functions are analytic. A constant linear relation on an open set would be an algebraic identity, contradicting the exact rank certificate. Their positive regulated Gram matrix is therefore nondegenerate.

Since the source interaction quotient has rank seven,

ker⁡(Isource(7)⟶Ophysical score)=0\boxed{ \ker\left( \mathcal I_{\rm source}^{(7)} \longrightarrow \mathcal O_{\rm physical\ score} \right)=0 }

at generic unequal energies before UV subtraction.

Result

the complete interaction score tower is physically faithful on the fixed source loop cycle.\boxed{ \text{the complete interaction score tower is physically faithful on the fixed source loop cycle.} }

This upgrades Entry 2460 from local moving-boundary representatives to the actual source cycle. It also shows that gradient-pivot denominators were pure coordinate artifacts.

Remaining analytic qualification

The loop integral is UV divergent and requires a declared subtraction scheme. The theorem concerns the regulated physical score Gram form. A subtraction can in principle collapse finite covectors; scheme-independent renormalized faithfulness is not inferred. Such a collapse would be a readout/renormalization obstruction, not new Carrier support unless it produced an independently derived divisor.

Durable evidence

Next falsifier

Apply a source-declared UV regulator and subtraction to the ten physical score covectors. Test whether their rank-seven quotient remains faithful in the finite part. Separate universal local counterterms from nonlocal elliptic periods before computing rank.

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