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Fig. D.1.

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A schematic representation of the angles involved in our radiative transfer calculations. The observer’s sightline (wave vector ) makes an angle θobs with respect to the jet/ axis. The magnetic field unit vector, , of an individual plasma cell is depicted in red. The radiative transfer is carried out in a cell-specific ‘Stokes U = 0’ linear polarization basis (depicted in blue). The cell-specific linear polarization basis is then rotated by an angle ϕrot onto a generalized observer’s plane (shown to the left).

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