Sari la conținut

Română · beta. Traducerea a fost făcută automat și este încă în curs de revizuire. Citește pagina în engleză

perspectiva aiqbenchCalcul cuantic

analiza aiqbench

This paper presents a rigorous mathematical analysis of local geometries within centered one-mode bosonic Gaussian covariances, specifically investigating the intersection points between Bures, Fisher-Rao, and Wasserstein determinants. The authors derive exact conditions for these metrics to cross at specific parameter values involving the golden ratio while distinguishing their operational implications regarding system unitaries versus Gaussian channels.
Sursă care acoperăarXiv
Ce este aceastaLectura unui model asupra articolului și a acoperirii conexe, scrisă pentru aiqbench. Nu sunt cuvintele publicației.

The Golden Junction of Gaussian Covariance Geometries: Sector Anisotropy, Relative-Entropy Response, and Local Penalties

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2609.17574v1 Announce Type: new Abstract: We compare four local geometries of centered one-mode bosonic Gaussian covariances while keeping their operational meanings distinct. In a common trace-orthonormal normalization, the Bures and covariance Fisher--Rao cometric determinants cross intrinsically at \(x^2=\varphi\). After introducing a constant action-matching parameter \(\eta\), the Bures--Wasserstein determinant joins them only at \((x,\eta)=(\sqrt\varphi,\sqrt\varphi)\). Equal determinant density does not mean tensor equality: relative to Fisher--Rao, the Bures cometric at the junction is \[ Q_{\rm gold}=\varphi^{-2}\Pi_0+\varphi\Pi_2, \qquad \det Q_{\rm gold}=1, \] so its inverse has the exact scalar-to-weight-two quadratic penalty ratio \(\varphi^3\). The normalized Bogoliubov--Kubo--Mori metric supplies an independent relative-entropy diagnostic. It agrees radially with Bures but has shape cometric eigenvalue \(4\hbar^2x/\log[(x+1)/(x-1)]\); it therefore does not form a fourth determinant junction and becomes tangentially stiff at the pure-state boundary. Operationally, weight-two motion is generated by a system-only Gaussian unitary, whereas radial motion requires a Gaussian channel or ancillary dilation. The known Uhlmann--Ruan purification quotient realizes the local Bures state metric, but an explicit \(\mathfrak{sp}(4,\mathbb R)\) test shows that an unweighted right-invariant Frobenius gate norm does not reproduce the golden penalty. Conditional branch selection and finite-rate Bures--Wasserstein cost separation are presented as secondary statements, not as dynamical phase transitions.

Abstract:We compare four local geometries of centered one-mode bosonic Gaussian covariances while keeping their operational meanings distinct. In a common trace-orthonormal normalization, the Bures and covariance Fisher--Rao cometric determinants cross intrinsically at \(x^2=\varphi\). After introducing a constant action-matching parameter \(\eta\), the Bures--Wasserstein determinant joins them only at \((x,\eta)=(\sqrt\varphi,\sqrt\varphi)\). Equal determinant density does not mean tensor equality: relative to Fisher--Rao, the Bures cometric at the junction is \[ Q_{\rm gold}=\varphi^{-2}\Pi_0+\varphi\Pi_2, \qquad \det Q_{\rm gold}=1, \] so its inverse has the exact scalar-to-weight-two quadratic penalty ratio \(\varphi^3\). The normalized Bogoliubov--Kubo--Mori metric supplies an independent relative-entropy diagnostic. It agrees radially with Bures but has shape cometric eigenvalue \(4\hbar^2x/\log[(x+1)/(x-1)]\); it therefore does not form a fourth determinant junction and becomes tangentially stiff at the pure-state boundary. Operationally, weight-two motion is generated by a system-only Gaussian unitary, whereas radial motion requires a Gaussian channel or ancillary dilation. The known Uhlmann--Ruan purification quotient realizes the local Bures state metric, but an explicit \(\mathfrak{sp}(4,\mathbb R)\) test shows that an unweighted right-invariant Frobenius gate norm does not reproduce the golden penalty. Conditional branch selection and finite-rate Bures--Wasserstein cost separation are presented as secondary statements, not as dynamical phase transitions.

arXiv:2609.17574 [quant-ph]

(or arXiv:2609.17574v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.17574 Focus to learn more arXiv-issued DOI via DataCite

arXivLabs is a framework that allows collaborators to develop and share new arXiv features directly on our website.

Both individuals and organizations that work with arXivLabs have embraced and accepted our values of openness, community, excellence, and user data privacy. arXiv is committed to these values and only works with partners that adhere to them.

Have an idea for a project that will add value for arXiv's community? Learn more about arXivLabs.

Text integral sub licența deschisă a publicației · 280 cuvinte

Subiecte conexe