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Geometric phase of arbitrary Mueller evolutions and its two-level quantum analogue

José J Gil

Abstract

We show that, for any physically realizable Mueller transformation -- including arbitrarily depolarizing maps -- the interferometric (Pancharatnam) geometric phase is fixed uniquely by the SO(3) rotation associated with the unitary (retarding) part of the pure characteristic component selected by the characteristic decomposition. All remaining characteristic contributions (discriminant and maximally mixed) can only reduce fringe visibility; they never generate geometric holonomy, even if their pure constituents involve rotations. We further establish the quantum analogue for open two-level dynamics: in the Choi representation of qubit channels, the geometric phase is fixed by the coherent unitary part of the dominant rank-one characteristic component, while the remaining dissipative structure affects visibility only.

Geometric phase of arbitrary Mueller evolutions and its two-level quantum analogue

Abstract

We show that, for any physically realizable Mueller transformation -- including arbitrarily depolarizing maps -- the interferometric (Pancharatnam) geometric phase is fixed uniquely by the SO(3) rotation associated with the unitary (retarding) part of the pure characteristic component selected by the characteristic decomposition. All remaining characteristic contributions (discriminant and maximally mixed) can only reduce fringe visibility; they never generate geometric holonomy, even if their pure constituents involve rotations. We further establish the quantum analogue for open two-level dynamics: in the Choi representation of qubit channels, the geometric phase is fixed by the coherent unitary part of the dominant rank-one characteristic component, while the remaining dissipative structure affects visibility only.
Paper Structure (14 equations)

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