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This paper advances the mathematical foundations of quantum information by establishing a fiber-bundle framework for fixed-rank density matrices, revealing rich topological structures like non-Abelian holonomy and Chern topology in mixed-state systems. By linking these geometric properties to physical phenomena such as decoherence-free subspaces and quantum Hall responses, the work provides new tools for diagnosing mixed-state matter beyond the limitations of full-rank approximations.
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Uhlmann Geometry of Fixed-Rank Density Matrices: A Fiber-Bundle Approach

arXiv3 min read

arXiv:2609.21875v1 Announce Type: new Abstract: For full-rank density matrices the state space is contractible, the Uhlmann bundle is topologically trivial, and the holonomy admits no quantized invariants; although the Uhlmann phase is genuinely geometric, this topological poverty has kept it from serving as a robust physical diagnostic of mixed-state matter. Mixed states of fixed rank below the Hilbert-space dimension, however, are ubiquitous: reduced states of subsystems, states in an invariant sector, and states in a decoherence-free subspace all have a support smaller than the Hilbert space that can vary with parameters. Their geometry is far richer: the support carries genuine curvature, non-Abelian holonomy, and Chern topology. We formulate Uhlmann's theory directly on the manifold of rank-$k$ density matrices: minimal purifications make the fixed-rank stratum the base of a principal $U(k)$-bundle whose Uhlmann connection is uniquely determined by a Sylvester equation, and in an eigenframe this connection takes a closed form reducing to the Berry, Wilczek--Zee, and faithful Uhlmann connections at $k=1$, at equal weights, and at $k=N$. The fixed-rank bundle inherits the topology of the Grassmannian, and non-factorizable higher Chern topology requires failure of the global eigenline splitting, which in the present spectral setting requires degeneracy, minimally realized by a rank-2 Yang monopole whose quantized second Chern number links the geometry to the four-dimensional quantum Hall response. Solvable models, from a genuinely non-Abelian holonomy to a decoherence-free Lindblad orbit, illustrate the content: the supporting subspace carries the topology, the spectral weights shape the transport, and the Uhlmann phase provides a direct geometric signature of these mixed-state phase transitions.

Abstract:For full-rank density matrices the state space is contractible, the Uhlmann bundle is topologically trivial, and the holonomy admits no quantized invariants; although the Uhlmann phase is genuinely geometric, this topological poverty has kept it from serving as a robust physical diagnostic of mixed-state matter. Mixed states of fixed rank below the Hilbert-space dimension, however, are ubiquitous: reduced states of subsystems, states in an invariant sector, and states in a decoherence-free subspace all have a support smaller than the Hilbert space that can vary with parameters. Their geometry is far richer: the support carries genuine curvature, non-Abelian holonomy, and Chern topology. We formulate Uhlmann's theory directly on the manifold of rank-$k$ density matrices: minimal purifications make the fixed-rank stratum the base of a principal $U(k)$-bundle whose Uhlmann connection is uniquely determined by a Sylvester equation, and in an eigenframe this connection takes a closed form reducing to the Berry, Wilczek--Zee, and faithful Uhlmann connections at $k=1$, at equal weights, and at $k=N$. The fixed-rank bundle inherits the topology of the Grassmannian, and non-factorizable higher Chern topology requires failure of the global eigenline splitting, which in the present spectral setting requires degeneracy, minimally realized by a rank-2 Yang monopole whose quantized second Chern number links the geometry to the four-dimensional quantum Hall response. Solvable models, from a genuinely non-Abelian holonomy to a decoherence-free Lindblad orbit, illustrate the content: the supporting subspace carries the topology, the spectral weights shape the transport, and the Uhlmann phase provides a direct geometric signature of these mixed-state phase transitions.

arXiv:2609.21875 [quant-ph]

(or arXiv:2609.21875v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.21875 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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