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arXiv:1508.02279 · Journal of Geometry and Physics

Purification of Lindblad dynamics, geometry of mixed states and geometric phases

David Viennot

Published Jul 17, 2018• 5 citations
arXivHTMLPDF
DOI
10.1016/j.geomphys.2018.06.019

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It is shown that Uhlmann's parallel transport of purifications along a path of mixed states represented by 2 × 2 density matrices is just the path-ordered product of Thomas rotations. These rotations are invariant under hyperbolic translations inside the Bloch sphere that can be regarded as the Poincaré ball model of hyperbolic geometry. A general expression for the mixed state geometric phase for an arbitrary geodesic triangle in terms of the Bures fidelities is derived. The formula gives back the solid angle result well known from studies of the pure state geometric phase. It is also shown that this mixed state anholonomy can be reinterpreted as the pure state non-Abelian anholonomy of entangled states living in a suitable restriction of the quaternionic Hopf bundle. In this picture Uhlmann's parallel transport is just the Pancharatnam transport of quaternionic spinors.
Dynamic quantum phase transitions (DQPT) following quantum quenches exhibit singular behavior of the overlap between the initial and evolved states. Here we present a formalism to incorporate a geometric phase into quench dynamics of mixed quantum states, a process named the Uhlmann quench, based on the Uhlmann parallel transport. To overcome the incompatibility between the Uhlmann parallel-transport condition and Hamiltonian dynamics, we formulate the evolution of purification of the density matrix in a form which not only respects the dynamics according to the density matrix but also follows the Uhlmann parallel-transport condition to generate a geometric phase after a quantum quench. For cyclic processes exemplified by a spin-1/2 system, geometric DQPTs (GDQPTs) can emerge with both singular behavior in the dynamic analog of the free energy and jumps of the geometric phase. Moreover, the Uhlmann phase reflecting the holonomy is generated at the end of each cycle. The Uhlmann quench thus paves the way for investigating the interplay between quantum dynamics and geometric processes in mixed states.
Geometric phases in quantum systems give rise to holonomies associated with cyclic evolution. In mixed-state settings, these holonomies arise from Uhlmann parallel transport on the purification bundle of density operators and depend on the global geometry of density-operator trajectories. In this work we introduce discretized mixed-state holonomy as a geometric encoding primitive. The public object is a density-operator trajectory, while the encoded information resides in a finite family of purification gauges associated with the same holonomy conjugacy class. By discretizing the gauge freedom of the purification bundle, continuous mixed-state holonomy is converted into finite alphabets suitable for discrete key spaces. We formalize the resulting primitive through an operational observation model and establish several structural properties. First, the holonomy representative cannot in general be reconstructed from the density-operator trajectory alone. Second, under conjugation-invariant observation channels, different encoded symbols are indistinguishable at the level of base-space observables. Third, discretized holonomy alphabets admit stable decoding under bounded perturbations of the underlying trajectory. The construction is illustrated through explicit qubit realizations based on isospectral mixed-state loops, together with representative-level decoding mechanisms and finite holonomy alphabets. We further discuss symmetry breaking, frame leakage, and limitations arising in realistic implementations. These results isolate a primitive-level geometric encoding mechanism based on mixed-state quantum geometry and provide a structural foundation for future cryptographic constructions involving representative-level holonomy information.