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C. Kerskens

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Preprint Jul 2026

Gaussian Purification Quotients and Fixed Nielsen Penalties

Information distance and circuit complexity are both obtained by minimizing lengths, but they minimize over different objects. We make this distinction explicit for faithful one-mode Gaussian states. First, invariant-form uniqueness implies that no positive-definite quadratic gate cost can be invariant under the full adjoint action of the noncompact symplectic group; a positive Cartan majorant necessarily introduces additional reference data. The Uhlmann purification quotient realizes the Bures metric, and the radial covariance direction requires a system-ancilla coupling because system-only Gaussian unitaries preserve the Williamson eigenvalue. We then minimize fixed right-invariant quadratic norms on the minimal two-mode Gaussian gate algebra \(\mathfrak{sp}(4,\mathbb R)\). For the unweighted Frobenius norm, the quotient coefficients for radial and traceless covariance tangents are $G_0=[\hbar^2(u-1)]^{-1}$ and $G_2=[\hbar^2(3u-1)]^{-1}$, where $u=(2\nu/\hbar)^2$. Their ratio does not equal the Bures ratio. The radial coefficient, however, reproduces the Bures value exactly at every $u$; the mismatch is confined to the traceless sector. More generally, a constant block-diagonal two-weight schedule gives $G_0/G_2=1+2(\beta/\alpha)u/(u-1)$; matching Bures throughout the isotropic family would require the state-dependent relation $\beta/\alpha=1/u$. At the Bures-Fisher determinant crossing \(u=\varphi\), pointwise matching is possible only by inserting $\beta/\alpha=\varphi^{-1}$. Thus the Bures purification quotient is an exact state-geometric cost, but it is neither an unweighted symplectic gate cost nor a member of this fixed two-weight Nielsen family. The existence of a more general fixed positive gate norm realizing the quotient remains open.

C. Kerskens · 0 citations
Preprint Jul 2026

The Quantum Correction to Gaussian Information Geometry is the Killing Form of the Symplectic Algebra

On the admissible cone $\mathcal C_\Omega=\{\Sigma\in\mathrm{Sym}^+(2n):\Sigma+i\Omega\ge0\}$ of Gaussian covariance matrices, the classical Bures--Wasserstein transport metric, the Fisher--Rao information metric, and the quantum Bures metric are individually well understood, but their mutual relationship is obscured by the operator equations defining them. Working with the contravariant (dual) metrics, we show that the exact difference between the dual quantum Bures metric and the dual Fisher--Rao metric is independent of the covariance matrix: it is identically the trace form, proportional to the Killing form, of the symplectic algebra $\mathfrak{sp}(2n,\mathbb R)$, pulled back through the isomorphism $X\mapsto\Omega X$. The signature of this form on the Cartan decomposition reproduces the anisotropic stiffening of the quantum metric at the pure-state boundary: it is negative on the compact subalgebra $\mathfrak u(n)$, which carries the divergence, and positive on the noncompact complement. Because the correction is quadratic in the momenta, a no-go lemma shows it cannot arise from minimal coupling to a principal connection. We realize it instead through a Schur complement of a pseudo-Riemannian metric on a phase bundle, whose base reduction is the quantum Bures metric and whose horizontal metric is the classical-limit Fisher--Rao metric. All identities are verified numerically to working precision.

C. Kerskens · 0 citations

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