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arXiv:2610.33848

Helstrom geometry with time-dependent spectral calibration

Kaushlendra Kumar

quant-phmath-phSubmitted Oct 24, 2026• Announced Oct 27, 2026• 0 citations
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Abstract

In a recent work we introduced a finite scalar-qubit-scalar spectral triple whose Connes distance reproduces the Bloch-ball trace metric up to a factor $2/Λ$, where $Λ^2=μ_L^2+μ_R^2$ for isotropic link strengths $μ_L,μ_R$ appearing in the proposed Dirac operator. Here we analyse time-dependent variation of these links, independent of the qubit dynamics. In doing so, we separate the distinguishability and calibration contributions to the spectral rate. A depolarizing example demonstrates spectral growth despite a monotonic contraction of the trace-distance. More generally, we characterize the admissible trace-distance histories compatible with a given positive spectral record and exhibit contracting and reviving realizations. At fixed $Λ$, we also study a sinusoidal link imbalance that preserves the Dirac spectrum and qubit metric, while the scalar-scalar distance oscillates with half the period of the imbalance.

AI Summary

The paper asks whether increasing Connes spectral distance witnesses quantum information backflow when the Dirac operator defining the metric varies independently of the qubit dynamics. It studies a finite scalar–qubit–scalar spectral triple with positive isotropic links $\mu_L(t),\mu_R(t)$. Building on the previously established identity $d(t)=2T(t)/\Lambda(t)$, where $T$ is trace distance and $\Lambda^2=\mu_L^2+\mu_R^2$, it separates distinguishability changes from calibration changes through $\dot d/d=\dot T/T-\dot\Lambda/\Lambda$. Explicit analytic constructions show that depolarizing evolution with $T(t)=T_0e^{-\gamma t}$ can exhibit spectral growth when the calibration scale decreases sufficiently quickly. More generally, for any positive differentiable spectral record on a finite interval, a differentiable trace-distance history is realizable by a common CPTP family and positive links if and only if $0<T(t)\leq T(0)\leq1$. Sufficiency follows from a random-unitary dephasing construction. Consequently, the same spectral record can describe either monotonic contraction or trace-distance revival. Simultaneous scalar-reference distances recover the missing calibration scale and hence $T(t)$. At fixed $\Lambda$, varying the link imbalance $\beta=\log(\mu_R/\mu_L)$ preserves both the Dirac spectrum and the qubit metric, while the scalar–scalar distance becomes $2\cosh\beta/\Lambda$. A sinusoidal imbalance therefore produces a scalar-distance oscillation at twice its frequency. The analysis assumes isotropic identity links and known spectral distances. Sampling-error propagation, physical implementation, and anisotropic links are left open; anisotropy need not admit the same scalar calibration.

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12 pages, 2 figures. Prepared for the proceedings of the XLIII Workshop on Geometric Methods in Physics (Białystok, Poland, 2026)

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In a recent work we introduced a finite scalar-qubit-scalar spectral triple whose Connes distance reproduces the Bloch-ball trace metric up to a factor 2/Λ2/Λ2/Λ, where Λ2=μL2+μR2Λ^2=μ_L^2+μ_R^2Λ2=μL2​+μR2​ for isotropic link strengths μL,μRμ_L,μ_RμL​,μR​ appearing in the proposed Dirac operator. Here we analyse time-dependent variation of these links, independent of the qubit dynamics. In doing so, we separate the distinguishability and calibration contributions to the spectral rate. A depolarizing example demonstrates spectral growth despite a monotonic contraction of the trace-distance. More generally, we characterize the admissible trace-distance histories compatible with a given positive spectral record and exhibit contracting and reviving realizations. At fixed ΛΛΛ, we also study a sinusoidal link imbalance that preserves the Dirac spectrum and qubit metric, while the scalar-scalar distance oscillates with half the period of the imbalance.
The paper asks whether increasing Connes spectral distance witnesses quantum information backflow when the Dirac operator defining the metric varies independently of the qubit dynamics. It studies a finite scalar–qubit–scalar spectral triple with positive isotropic links μL(t),μR(t)\mu_L(t),\mu_R(t)μL​(t),μR​(t). Building on the previously established identity d(t)=2T(t)/Λ(t)d(t)=2T(t)/\Lambda(t)d(t)=2T(t)/Λ(t), where TTT is trace distance and Λ2=μL2+μR2\Lambda^2=\mu_L^2+\mu_R^2Λ2=μL2​+μR2​, it separates distinguishability changes from calibration changes through d˙/d=T˙/T−Λ˙/Λ\dot d/d=\dot T/T-\dot\Lambda/\Lambdad˙/d=T˙/T−Λ˙/Λ.
Explicit analytic constructions show that depolarizing evolution with T(t)=T0e−γtT(t)=T_0e^{-\gamma t}T(t)=T0​e−γt can exhibit spectral growth when the calibration scale decreases sufficiently quickly. More generally, for any positive differentiable spectral record on a finite interval, a differentiable trace-distance history is realizable by a common CPTP family and positive links if and only if 0<T(t)≤T(0)≤10<T(t)\leq T(0)\leq10<T(t)≤T(0)≤1. Sufficiency follows from a random-unitary dephasing construction. Consequently, the same spectral record can describe either monotonic contraction or trace-distance revival. Simultaneous scalar-reference distances recover the missing calibration scale and hence T(t)T(t)T(t).
At fixed Λ\LambdaΛ, varying the link imbalance β=log⁡(μR/μL)\beta=\log(\mu_R/\mu_L)β=log(μR​/μL​) preserves both the Dirac spectrum and the qubit metric, while the scalar–scalar distance becomes 2cosh⁡β/Λ2\cosh\beta/\Lambda2coshβ/Λ. A sinusoidal imbalance therefore produces a scalar-distance oscillation at twice its frequency.
The analysis assumes isotropic identity links and known spectral distances. Sampling-error propagation, physical implementation, and anisotropic links are left open; anisotropy need not admit the same scalar calibration.
We show that the equal-prior Helstrom trace-distance geometry of qubit states is recovered from Connes spectral distance in a finite scalar-qubit-scalar model. The two scalar reference sectors couple isotropically to the qubit block through identity Dirac links, so that the full Bloch ball, including mixed states, inherits its standard chordal trace-distance geometry from the finite spectral metric. The scalar-sector distances serve a distinct calibration role: they determine the individual link lengths, satisfy a Pythagorean consistency relation, and reconstruct the middle-sector scale.
In this paper, we study the properties of Connes spectral distances between quantum states under unitary transformations. We mainly focus on spectral triples with matrix algebras acting on finite dimensional Hilbert spaces. We prove that there are some finite spectral triples in which the Lipschitz seminorms are equal to the operator norms. We also explicitly construct some spectral triples in which the Connes spectral distances between quantum states are exactly the quantum trace distances. These results are helpful for us to better study the relationships among Connes spectral distance, quantum trace distance and other quantum distance measures. These concrete examples are significant for studies of geometric structures of finite spectral triples and mathematical relations of qubits and other quantum states in the framework of noncommutative geometry.
The Bures--Helstrom metric is the minimal monotone Riemannian metric on the state space of a qubit. With the quantum Fisher normalization used here, it identifies the Bloch ball with a geodesic hemisphere of the unit round three--sphere. We describe its Ricci flow explicitly. In a general rotationally symmetric gauge the flow is a coupled system for the radial lapse and warping factor; a single scalar equation appears only after a Hamilton--DeTurck gauge choice. In the corresponding moving DeTurck frame the squared warping function Ψ=Φ2Ψ=Φ^2Ψ=Φ2 satisfies the linear forced heat equation \begin{equation*} D_tΨ=Ψ_{ss}-2, \end{equation*} while the fixed-lapse coordinate form contains the associated transport term. Since the Bures--Helstrom metric is Einstein, the geometric flow itself is the homothetic shrinker \begin{equation*} g(t)=(1-4t)g_{\mathrm{BH}}, \end{equation*} with scalar curvature 6/(1−4t)6/(1-4t)6/(1−4t) and extinction time T=1/4T=1/4T=1/4. Thus the metric remains inside the monotone cone for all t<Tt<Tt<T and leaves the cone of nondegenerate Riemannian metrics only through the collapsed limit. We also record the volume--normalized flow, for which the Bures--Helstrom metric is a fixed point. Its linearization is the shifted round--sphere Laplacian ΔS3+3Δ_{\mathbb S^3}+3ΔS3​+3, with spectrum \begin{equation*} σ_\ell=-(\ell-1)(\ell+3), \end{equation*} and spectral gap 555 after removal of the scaling mode.
Spectral constraints can alter the observable manifestation of quantum geometry without changing the local eigenspace. Relativistic electron vortices provide a sharp example: the spin orbit interaction redistributes spin and orbital angular momentum, yet its magnetic contribution differs between localized three-dimensional wave packets and stationary monochromatic beams. We resolve this discrepancy by showing that fixing the energy replaces ambient momentum derivatives in position-weighted current moments by shell-tangent derivatives and derive a Hermitian selection rule for first-order observables in momentum-dependent internal subspaces. Its extension-independent form applies beyond Dirac systems, including a broad class of antisymmetric first moments of scalar-charge velocity currents. For the free positive-energy Dirac doublet, the magnetic correction is an exact non-Abelian Berry-curvature contraction with a pointwise saturable quantum-metric bound. Changing the relative phase between the two σzσ_zσz​ spinor components switches this correction from zero in a conserved transverse-helicity sector to a finite value in a radial coherent superposition. At fixed finite Lorentz factor, the radial response scales as O(θ/γ)O(θ/γ)O(θ/γ), compared with O(θ2)O(θ^2)O(θ2) for longitudinal polarization. Spectral reduction and internal coherence thus provide distinct controls of the observable imprint of quantum geometry.
Abstract We construct spectral triples of one- and two-qubit states using the Hilbert-Schmidt operatorial formulation, and study the Connes spectral distances. We also construct the Dirac operator corresponding to the normal quantum trace distances. Based on the Connes spectral distances, we propose some definitions of quantum discord and coherence measure of quantum states, and explicitly calculate the coherence of one-qubit states. We also study some simple cases about two-qubit states, and the corresponding spectral distances satisfy the Pythagoras theorem. These results are significant for studies on physical relations and geometric structures of qubits and other quantum states.
We study the geometric spread of discrete-time quantum walks using Connes' distance formula. We introduce its discrete analogue by adapting the continuous spectral metric to the lattice, with the Dirac operator replaced by the unitary step operator. Focusing first on a (2+1)-dimensional quantum walk, we evaluate the dynamical spread of localized wavepackets to compare propagation in free space against that under a uniform magnetic field. We find that while the free walk shows linear ballistic growth, gauge-induced phases in the magnetic walk constrain the admissible test operators, suppressing the long-time geometric expansion. Furthermore, we apply this discrete framework to a (1+1)-dimensional plastic quantum walk simulating an inhomogeneous spatial metric. The results demonstrate that the discrete Connes distance naturally captures the underlying spatially varying metric, providing a robust measure of the wavepacket's spread that adapts directly to the local simulated geometry.