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The question of the representation of quantum stationary partially polarizedwaves as random superpositions of different polarization ellipses is addressed.To this end, the Bohmian formulation of quantum mechanics is considered andextended to quantum optical polarization. As is shown, this approach properlycombines definite time-evolving trajectories with rigorous stationary quantumdistributions via the topology displayed by the associated phase field.

Reconciling quantum trajectories and stationary quantum distributions in single-photon polarization states