Table 4.
Geometry transition properties of individual sources.
| Name | Class | xb/mas (xb/pc) | Rj(xb)/mas | lin | lout | θ/deg |  |
 |
rB/(mas) (rB/(pc)) |
|---|---|---|---|---|---|---|---|---|---|
| 3C 66A | B | 2.31 ± 0.32 (65) | 0.42 ± 0.14 | 0.56 ± 0.13 | 1.33 ± 0.11 | 9.8 (a) | 4.0 (326) | 8.1(328) | 0.046 − 1.255 (1.31 − 35.51) |
| CTA 26 | Q | 2.12 ± 0.26 (293) | 0.68 ± 0.15 | 0.62 ± 0.12 | 1.78 ± 0.27 | 3.2 (b) | 16.8 (119) | 21.3 (121) | 0.0011 − 0.0310 (0.16 − 4.27) |
| 3C 111 | G | 5.42 ± 0.29 (16) | 0.56 ± 0.09 | 0.60 ± 0.08 | 1.69 ± 0.24 | 19.0 (c) | 12.1 (662) | 12.8 (664) | 0.23 − 6.55 (0.67 − 19.07) |
| PKS 0528+134 | Q | 2.10 ± 0.38 (596) | 0.56 ± 0.16 | 0.54 ± 0.11 | 1.24 ± 0.25 | 1.7 (b) | 10.0 (336) | 10.9 (338) | 0.0035 − 0.0925 (0.99 − 26.32) |
| 4C +71.04 | Q | 2.75 ± 0.41 (413) | 0.35 ± 0.13 | 0.48 ± 0.14 | 1.15 ± 0.15 | 3.2 (b) | 15.7 (139) | 19.0 (141) | 0.0018 − 0.0495 (0.28 − 7.42) |
| Mrk 421 | B | 1.93 ± 0.38 (13 − 34) | 0.63 ± 0.19 | 0.54 ± 0.13 | 1.02 ± 0.13 | (2 − 5) (d) | 10.1 (253) | 11.5 (255) | 0.0048 − 0.3522 (0.084 − 2.456) |
| 4C +29.45 | Q | 2.52 ± 0.60 (522) | 0.91 ± 0.37 | 0.73 ± 0.17 | 1.23 ± 0.21 | 2.0 (b) | 8.5 (84) | 9.3 (86) | 0.0034 − 0.0918 (0.084 − 2.456) |
| 3C 279 | Q | 0.61 ± 0.22 (97) | 0.15 ± 0.09 | 0.49 ± 0.15 | 0.78 ± 0.09 | 2.4 (b) | 33.1 (390) | 33.8 (392) | 0.012 − 0.337 (1.98 − 53.74) |
| BL Lac | B | 1.97 ± 0.13 (20) | 0.37 ± 0.07 | 0.78 ± 0.09 | 1.97 ± 0.08 | 7.5 (b) | 9.6 (1058) | 17.0 1060 | 0.046 − 1.184 (0.46 − 11.76) |
Notes. Columns: (1) Common name, (2) Classification, (3) geometry break point in angular scale (geometry break point in linear scale deprojected), (4) Jet radius at the break point, (5) lin, (6) lout, (7) inclination angle, (8) 
for the broken power law fit, (9) 
for the single power law fit. (10) Range of plausible Bondi radii in angular scale (range of plausible Bondi radii in linear scale deprojected)
References. (a) Hovatta et al. (2009), (b) Pushkarev et al. (2009), (c) Kadler et al. (2008), (d) Lico et al. (2012).
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