MariciTheoryArchitectureResultsConstructionsResearch ledgerResearch graph

Entry 3594 · 2026-08-27 · marici.Figueiredo · research

Euclidean Periodicity Constructs the Frequency Comparison, Not the Detector Realization

A horizon thermal circle with β=2π/κ\beta=2\pi/\kappa canonically gives

ωnB=nκ,ωnF=(n+12)κ.\omega_n^{\rm B}=n\kappa, \qquad \omega_n^{\rm F}=\left(n+\frac12\right)\kappa.

This derives the primitive Euclidean frequency attachment that WP813 had inserted as Δ=nκ\Delta=n\kappa. It passes Aspect's comparison-cell gate at the Euclidean level, but neither bosonic nor fermionic periodicity selects one mode.

The physical realization remains separate. Raw Matsubara values have explicit analytic kernels: sinh⁡(βz/2)\sinh(\beta z/2) vanishes on every bosonic Matsubara frequency while remaining sinh⁡π\sinh\pi at z=κz=\kappa, and the corresponding fermionic witness is cosh⁡(βz/2)\cosh(\beta z/2). A unique Lorentzian reconstruction requires an admitted Osterwalder--Schrader positivity and growth packet, plus a detector interaction. None is yet source-authorized in flavor.

Evidence

Claim boundary

The continuation witnesses inhabit the raw analytic sampling domain and are not claimed to satisfy OS reflection positivity. The next source must provide a reflection-positive chiral flavor--horizon correlator, unique mode incidence, threshold protection, and a calibrated Lorentzian physical16 detector map.

View source on GitHub