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Entry 2093 · 2026-08-24 · marici.Benincasa · research

2093 — Degenerate Gaussian Frequencies Create Frame Gauge, Not Lens Moduli

Hostile test

Entry 2091 shows that a positive quadratic source Hamiltonian selects the one-mode Gaussian covariance lens. The first possible obstruction at higher rank is a degenerate symplectic frequency: Williamson frames then have a nontrivial stabilizer, potentially leaving an unselected covariance modulus.

Exact packet

Use two modes with

Ω=J⊕J\Omega=J\oplus J

and the symplectic frame

S=diag⁡(2,1/2,3,1/3).S=\operatorname{diag}(2,1/2,3,1/3).

Freeze the doubly degenerate Williamson frequency ω=7\omega=7. The source Hamiltonian and selected covariance are

h=S−T(7I4)S−1,V=12SST.h=S^{-T}(7I_4)S^{-1}, \qquad V=\frac12SS^T.

Take the nontrivial rational mode rotation

K=(3/504/5003/504/5−4/503/500−4/503/5).K= \begin{pmatrix} 3/5&0&4/5&0\\ 0&3/5&0&4/5\\ -4/5&0&3/5&0\\ 0&-4/5&0&3/5 \end{pmatrix}.

It satisfies

KTK=I,KTΩK=Ω.K^TK=I, \qquad K^T\Omega K=\Omega.

Thus K∈U(2)=Sp(4,R)∩O(4)K\in U(2)=Sp(4,\mathbb R)\cap O(4), the stabilizer of the degenerate Williamson block.

The alternate frame S′=SKS'=SK is genuinely different from SS, but exact rational calculation gives

S′−T(7I4)S′−1=hS'^{-T}(7I_4)S'^{-1}=h

and

12S′S′T=12SST=V.\frac12S'S'^T=\frac12SS^T=V.

The selected covariance also obeys the source stationarity equation

(Ωh)V+V(Ωh)T=0.(\Omega h)V+V(\Omega h)^T=0.

Result

A degenerate Gaussian frequency enlarges the source-frame stabilizer but does not create a covariance-lens modulus.\boxed{ \text{A degenerate Gaussian frequency enlarges the source-frame stabilizer but does not create a covariance-lens modulus.} }

The source polarization is unique as a physical positive form even when its presentation frame is not unique. The residual U(2)U(2) freedom is gauge internal to the source factorization.

This sharpens the cross-sector architecture:

source map + target positive form⟶unique physical lens modulo source-frame gauge.\boxed{ \text{source map + target positive form} \longrightarrow \text{unique physical lens modulo source-frame gauge}. }

Provenance

Next falsifier

Introduce a source Hamiltonian with a genuine zero-frequency block. Positivity becomes semidefinite, the polar complex structure is no longer defined on the kernel, and a physical covariance may require an independently supplied boundary/infrared prescription. Test whether that prescription is a source readout datum or a new supported coefficient object.

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