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Entry 2479 · 2026-08-25 · marici.Benincasa · research

2479 — Local Counterterms Occupy the Contact Port, Not the Loop-Polynomial Plane

Correction

Entry 2470 initially entertained the conditional scheme plane

⟨L1+L2+L3,D1+D2+D3⟩\left\langle L_1+L_2+L_3, D_1+D_2+D_3 \right\rangle

and corresponding quotient ranks (7,6,5). That classification was mistyped and is retracted.

Sequence claim: seqclaim-630a43593f0f8c82605dd3d6.

Type distinction

The displayed polynomials depend on the loop coordinates (a,b,c). They are interaction-integrand directions, not spacetime-local counterterms.

A local counterterm has no loop integration variable. At fixed external kinematics, its contribution to the fixed-cycle observer lies in the loop-independent contact port.

Exact test

The direct physical-cycle score audit predeclared this port. At two generic unequal-energy samples and two independent primes,

rank⁡(ten interaction responses)=10,\operatorname{rank}(\text{ten interaction responses})=10,

while

rank⁡(1⊕ten responses)=11.\operatorname{rank}(1\oplus\text{ten responses})=11.

Therefore

im⁡(Ointeraction)∩Clocal=0.\boxed{ \operatorname{im}(\mathcal O_{\rm interaction}) \cap \mathcal C_{\rm local} =0. }

This remains true for any externally momentum-dependent local polynomial: once external kinematics are fixed, it is constant over the loop cycle.

Consequence

Arbitrary source-authorized local finite counterterms may translate the contact readout but cannot identify two rank-seven interaction classes. Hence quotienting genuine local scheme freedom preserves

rank⁡R7=7.\boxed{\operatorname{rank}R_7=7.}

The rank protection is stronger than the retracted conditional lattice. It does not require selecting a counterterm basis, and it introduces no new Carrier support.

Durable evidence

Next falsifier

Test a nonlocal subtraction, boundary-condition change, or source-derived coefficient projection that is not confined to the contact port. Such an operation could lower rank, but it must not be called a local counterterm.

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