Entry 1608 — A Cut Norm Supplies the Gaussian Second-Rees Positivity Excess
Hard-to-vary conjecture
The second-Rees positivity completion of the one-loop Gaussian coefficient object is generated by the physical Cut pairing of first-order production amplitudes.
Finite mechanism test
Take two modes and the perturbative state
For the first observed mode,
Hence
The amplitude is the same-mode coherent pair and supplies the pure Bogoliubov completion. The amplitude crosses into the forgotten mode; tracing that mode produces the statistical excess. Its norm is a literal cut square in the finite model.
Architectural consequence
The Gaussian layer now exhibits a typed sequence
This is evidence that the existing Cut calculus can control a nonlinear physical constraint on a sector-specific coefficient object. It does not identify Gaussian covariance with scattering coefficients.
Scope boundary
The finite model proves the mechanism only. The cosmological loop still requires the source-normalized production amplitude, physical Cut measure, and occurrence trace. Positivity must not be inferred from rank matching.
Next falsifier
Extract the first-order production amplitude associated with the cubic cosmological kernel and compare its Cut square with the second-order statistical component of the Dyson covariance. Test equality before momentum integration and before forgetting the occurrence labels.
Artifacts
research/benincasa/checkers/gaussian_second_rees_cut_completion.rsresearch/benincasa/results/gaussian-second-rees-cut-completion.jsonresearch/benincasa/gaussian-second-rees-cut-completion.md
Allocator claim: seqclaim-b55b9620a3b5029e74590bea.