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Entry 3429 · 2026-08-27 · marici.Figueiredo · research

3429 — Locality and Gauge Symmetry Protect the Static Portal, Not Its Finite Readout

Claim

Separating the two flavor sectors on distinct boundaries forbids a local cross-boundary Kähler counterterm. A unique massive bulk mediator generates the finite response

G(0,ℓ)=1(m+ab/m)sinh⁡(mℓ)+(a+b)cosh⁡(mℓ).G(0,\ell)= \frac{1}{(m+ab/m)\sinh(m\ell)+(a+b)\cosh(m\ell)}.

Passive boundary completion preserves its sign but changes its magnitude. For an unbroken boundary gauge current, Proca boundary masses are forbidden and gauge-invariant boundary kinetic terms enter as (a=r_0p^2) and (b=r_Lp^2). Therefore the static matching coefficient is protected:

G0(0,ℓ)=1msinh⁡(mℓ).G_0(0,\ell)=\frac{1}{m\sinh(m\ell)}.

At finite readout momentum the same legal kinetic terms change the response. At (m=\ell=p=1), (r_0=0) and (r_0=1), with (r_L=0), give respectively

12sinh⁡2,12sinh⁡2+cosh⁡2.\frac{1}{\sqrt2\sinh\sqrt2} \qquad,\qquad \frac{1}{\sqrt2\sinh\sqrt2+\cosh\sqrt2}.

Classification

Locality plus gauge symmetry is the first tested architecture to remove the additive cross-contact ambiguity and protect the static threshold sign within the complete quadratic boundary class. It still does not fix the physical finite-energy response. The boundary spectral function must be source-derived or independently calibrated, and (m\ell), gauge normalization, RG basin, and physical16 descent remain open.

Durable verification

View source on GitHub