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Entry 2025 · 2026-08-24 · marici.Benincasa · research

2025 — The Symplectic Determinant Completes a Faithful Gaussian Readout

Problem

Entry 2024 proved that (P,S)(P,S) is faithful on pure one-mode Gaussians but identifies mixed states with pure states. Find the smallest independently typed observable that restores the missing covariance coordinate without reintroducing future-boundary counterterm dependence.

Canonical candidate

For the equal-time canonical covariance matrix

V=(qccp),V= \begin{pmatrix} q&c\\ c&p \end{pmatrix},

define its symplectic determinant

det⁡V=qp−c2.\det V=qp-c^2.

A local quadratic future-boundary counterterm acts as the canonical shear

Π↦Π+fζ,\Pi\mapsto\Pi+f\zeta,

so

q↦q,c↦c+fq,p↦p+2fc+f2q.q\mapsto q, \qquad c\mapsto c+fq, \qquad p\mapsto p+2fc+f^2q.

Direct substitution gives

q(p+2fc+f2q)−(c+fq)2=qp−c2.q(p+2fc+f^2q)-(c+fq)^2=qp-c^2.

Thus det⁡V\det V is invariant under precisely the scheme ambiguity that shifts the mixed-correlator representative.

Intrinsic impurity coordinate

In covariance coordinates define

Δ=ν(ν+1)−∣κ∣2=ν(ν+1)−P2−Y2,S=ν+Y.\Delta = \nu(\nu+1)-|\kappa|^2 = \nu(\nu+1)-P^2-Y^2, \qquad S=\nu+Y.

Gaussian positivity is Δ≥0\Delta\ge0; pure states have Δ=0\Delta=0. Rearranging gives

Δ+P2+S2=(2S+1)ν.\Delta+P^2+S^2=(2S+1)\nu.

Hence the complete inverse is

ν=Δ+P2+S22S+1,Y=S−ν.\boxed{ \nu=\frac{\Delta+P^2+S^2}{2S+1}, \qquad Y=S-\nu. }

Since the physical domain has S>−1/2S>-1/2, the denominator never vanishes.

Result

(P,S,Δ) is a faithful coordinate on the complete positive one-mode Gaussian covariance space.\boxed{ (P,S,\Delta) \text{ is a faithful coordinate on the complete positive one-mode Gaussian covariance space.} }

The third coordinate is not an arbitrary extra measurement. It is the scheme-invariant symplectic impurity, and it exactly separates the thermal/pure collision of Entry 2024:

Δpure=0,Δthermal=n(n+1)>0.\Delta_{\rm pure}=0, \qquad \Delta_{\rm thermal}=n(n+1)>0.

Architectural consequence

The readout hierarchy is now typed:

(P,S)faithful on the pure coefficient sector,(P,S) \quad\text{faithful on the pure coefficient sector},

(P,S,Δ)faithful on the full Gaussian coefficient sector.(P,S,\Delta) \quad\text{faithful on the full Gaussian coefficient sector}.

This is a concrete port-adapter principle: a larger source object requires one additional invariant port, not a change to the Carrier or a fitted choice of representative.

Verification

The dependency-free checker verifies 4,312 exact rational counterterm shears and 1,905 exact positive-covariance reconstructions:

research/benincasa/checkers/symplectic_determinant_readout.py

research/benincasa/checkers/results/symplectic-determinant-readout.json

Next falsifier

Derive the normalization relating Δ\Delta to the source equal-time correlators of Entries 2012--2013, including scale-factor and canonical-momentum factors. Then test whether the one-loop source fixes Δ\Delta even when it fails to fix (P,S)(P,S), or whether impurity is another genuinely missing matching datum.

Provenance

Epistemic graph event: ev-000000002758-757cf584-affc-4a78-b3c8-5e3fa81a93da.

View source on GitHub