“…Thanks to the FM, both and can be neglected. Since the polarization properties are reciprocal in the fiber bundle section, the FM compensates for their effect [ 8 ]. The equation can then be rewritten as where , , and correspond to a spun fiber section whose Jones matrix can be generally expressed as a retarder-rotator pair, yielding [ 12 ] where l is the spun fiber length, the retardance, is the angle of the retarder’s fast eigenmode, and is the rotation angle of the rotator.…”