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Table A.1

continued.

ID S [Jy] d [mas] θ b maj log TB
J4 0.15 39.72 49.05 2.30 8.71
J3 0.04 52.66 50.69 0.64 9.18
J2a 0.02 59.91 49.17 0.38 9.30
J2b 0.05 63.81 49.50 0.82 9.07
0.03 94.26 51.31 1.46 8.43
2009-12-13 (χ2 = 2232.0, d.o.f. = 2350)
0.05 45.12 −128.14 3.24 7.93
0.09 13.72 −128.52 0.63 9.57
0.35 3.81 −121.34 0.52 10.36
Core 1.76 0.00 – 0.72 10.77
Jstat 0.84 3.27 43.42 0.72 10.45
J8 0.31 10.11 55.31 0.74 9.99
J7 0.33 13.56 49.15 1.89 9.21
0.12 24.47 41.03 2.67 8.48
J4 0.07 39.89 49.11 2.59 8.23
2010-07-24 (χ2 = 5250.3, d.o.f. = 8642)
0.02 68.35 −124.16 4.42 7.25
0.07 20.74 −123.58 4.32 7.80
0.06 9.55 −136.56 3.08 8.07
0.06 1.21 −113.38 < 0.02 > 12.2
Core* 0.78 0.22 −44.02 0.47 10.79
Core* 0.75 0.21 135.98 0.49 10.74
Jstat 0.69 2.83 46.61 0.79 10.29
J10 0.40 4.79 43.70 0.89 9.95
J9 0.19 7.56 47.80 0.63 9.93
J8 0.26 12.43 49.88 1.92 9.08
J7 0.34 16.60 50.64 3.32 8.73
J6 0.03 21.66 46.42 0.63 9.10
0.09 22.15 54.23 0.71 9.48
0.11 26.72 51.16 0.70 9.59
0.08 31.63 49.86 0.78 9.35
J5 0.12 36.57 48.39 1.12 9.23
J4 0.12 40.43 47.11 2.34 8.57
J3 0.03 58.10 53.89 3.41 7.63
2011-04-01 (χ2 = 23905.7, d.o.f. = 6846)
0.07 111.32 −126.36 3.55 7.96
0.20 55.99 −123.57 9.71 7.56
0.05 39.70 −124.57 0.56 9.48
0.08 36.29 −122.40 2.89 8.20
0.06 23.94 −124.06 0.40 9.83
0.36 9.75 −131.91 3.45 8.73
0.46 1.65 −127.32 0.57 10.40
0.23 0.48 −81.91 0.04 12.41
Core 0.85 0.00 – 0.47 10.84
0.84 1.66 44.80 0.62 10.58
Jstat 0.82 4.19 46.56 0.65 10.53
J10 0.31 7.39 49.16 0.58 10.21
J9 0.21 10.54 48.63 0.88 9.66
J8 0.23 13.60 49.24 2.50 8.82
0.20 15.09 49.13 0.74 9.80
J7 0.21 17.97 46.48 2.50 8.76
J6 0.10 24.39 45.40 0.58 9.72
0.06 32.64 47.70 0.57 9.53
0.12 36.16 47.26 0.57 9.80
J5 0.14 39.54 47.53 0.75 9.64
J4 0.13 47.58 48.38 2.02 8.74
J3 0.15 61.70 48.80 2.21 8.73
0.15 105.84 47.61 3.60 8.31

Notes.

(*)

Due to the complex structure of the core region, a stable model requires two close components which are strongly correlated. Their flux weighted central point was taken as a reference position.

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