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Table B.1.

Polarization degree and EVPA for different jet shapes and emission scenarios.

Jet shape Emission scenario Πmin Πmax ΔΠ Ψmin Ψmax ΔΨ
Cylindrical single blob 0.789 0.789 0 1.050 2.092 1.042
single blob + jet 0.610 0.782 0.172 1.190 1.952 0.762
multiple blobs 0.412 0.788 0.376 1.077 2.046 0.969
multiple blobs + jet 0.578 0.738 0.160 1.348 1.778 0.430

“Sausage-like” C2 = 0.8 single blob 0.789 0.789 0 0.909 2.262 1.353
single blob + jet 0.520 0.782 0.262 1.081 2.163 1.082
multiple blobs 0.238 0.788 0.550 0.900 2.254 1.354
multiple blobs + jet 0.493 0.741 0.248 1.317 1.966 0.649
“Sausage-like” C2 = 2 single blob 0.789 0.789 0 -9.061 5.321 14.382
single blob + jet 0.170 0.766 0.596 0.876 2.345 1.469
multiple blobs 0.023 0.779 0.756 -4.672 2.192 6.864
multiple blobs + jet 0.034 0.654 0.620 0.832 2.283 1.451

Nearly parabolic single blob A 0.789 0.789 0 -1.083 5.004 6.087
single blob A + jet 0.121 0.777 0.656 -0.259 1.805 2.064
single blob B 0.789 0.789 0 0.998 2.443 1.445
single blob B + jet 0.075 0.769 0.694 0.135 2.360 2.225
multiple blobs 0.063 0.785 0.722 0.810 6.786 5.976
multiple blobs + jet 0.021 0.722 0.701 0.890 6.727 5.837

Notes. We report the minimum and maximum values of the polarization degree, Π, and EVPA, Ψ (measured in radians), for each jet shape and emission scenario, over the entire observation period, tobs = 20 days. We define ΔΠ = Πmax − Πmin and ΔΨ = Ψmax − Ψmin. The time evolution of the cylindrical jet is shown in Fig. 3, the time evolution of the “sausage-like” jet is shown in Figs. 45, and the time evolution of the nearly parabolic jet is shown in Fig. 6. When the jet is nearly parabolic, “single blob A” and “single blob B” correspond to different initial coordinates of the blob, as reported in Table 1.

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