“…Two experimental approaches have been used to rotate the polarization of the probing light, using PEMs and EOMs. The PEM [50,76] provides a sinusoidal phase change δ ∝ sin(ωt), while the EOM [28,48,77,78] is characterized by a linear phase change δ ∝ ωt. The respective Jones matrices are reported in Table 10.2.…”