Table 5.
Sample of sources considered for the analysis in Sect. 4, sorted by redshift.
B1950 | Other | z | Class | log MBH | LX/LEdd | Accretion | pc/mas | RS/mas | θ | k | zt |
---|---|---|---|---|---|---|---|---|---|---|---|
name | name | [M⊙] | mode | [deg] | [mas] | ||||||
1228+126 | M 87 | 0.0043 | RG | 9.81[1] | 2.7e−8[15] | LEG | 0.087 | 140 | 16[22] | ∼0.57[44] | 131 |
0238-084 | NGC 1052 | 0.0050 | RG | 8.19[2] | 2.1e−5[16] | LEG | 0.102 | 6880 | 49[23] | 0.39 ± 0.05[34] | 3.73 |
1216+060 | NGC 4261 | 0.0074 | RG | 8.69[3] | 8.4e−7[15] | LEG | 0.150 | 3201 | 63[24] | 0.62 ± 0.13[45] | ∼4.5 |
0055+300 | NGC 315 | 0.0165 | RG | 9.12[4] | 3.7e−6[17] | LEG | 0.331 | 2662 | 38[25] | 0.45 ± 0.15 | 1.07 |
0316+413 | 3C 84 | 0.0176 | RG | 8.49[2] | 1.3e−4[15] | LEG | 0.352 | 11910 | 18[26] | 0.50 ± 0.03[23] | – |
0313+411 | IC 310 | 0.0189 | BL | 8.48[5] | − | LEG | 0.379 | 13208 | 15[27] | 2.30 ± 0.10[34] | – |
1142+198 | 3C 264 | 0.0217 | RG | 8.67[6] | 1.2e−5[15] | LEG | 0.433 | 9673 | 10[28] | 0.66 ± 0.02[29] | ∼4.5 |
1637+826 | NGC 6251 | 0.0247 | RG | 8.78[7] | 7.4e−5[15] | LEG | 0.491 | 8513 | 19[29] | 0.51 ± 0.04[34] | 2.13 |
0305+039 | 3C 78 | 0.0287 | RG | 8.60[2] | 4.5e−5[15] | LEG | 0.567 | 14894 | 20[30] | 0.99 ± 0.12[34] | – |
1101+384 | Mrk 421 | 0.0300 | BL | 8.29[2] | − | LEG | 0.593 | 31794 | 4[31] | 1.49 ± 0.11[34] | – |
0430+052 | 3C 120 | 0.0330 | RG | 7.74[8] | 1.4e−2[18] | HEG | 0.650 | 122446 | 19[23] | 0.56 ± 0.07[34] | 2.85 |
1652+398 | Mrk 501 | 0.0337 | BL | 9.21[2] | − | LEG | 0.662 | 4272 | 4[32] | 0.57 ± 0.02[34] | – |
2344+514 | 1ES 2344+514 | 0.0440 | BL | 8.80[2] | − | LEG | 0.855 | 14166 | 2[33] | 1.33 ± 0.15[34] | – |
1133+704 | Mrk 180 | 0.0453 | BL | 8.21[2] | − | LEG | 0.879 | 56728 | 5[34] | 0.53 ± 0.04[34] | 1.46 |
1959+650 | 1ES 1959+650 | 0.0470 | BL | 8.09[2] | − | LEG | 0.910 | 77350 | 2[35] | 0.81 ± 0.26[34] | – |
1514−241 | AP Librae | 0.0490 | BL | 8.10[2] | − | LEG | 0.947 | 78579 | 6[36] | 1.10 ± 0.06[34] | – |
0415+379 | 3C 111 | 0.0485 | RG | 8.26[9] | 5.1e−3[18] | HEG | 0.937 | 54424 | 17[23] | 0.47 ± 0.03[34] | 7.07 |
1807+698 | 3C 371 | 0.0510 | BL | 8.51[2] | − | LEG | 0.983 | 31720 | 7[23] | 0.39 ± 0.09[34] | 1.67 |
1514+004 | PKS 1514+00 | 0.0525 | RG | 7.50[10] | 2.8e−3[19] | HEG | 1.010 | 334163 | 15[34] | 0.56 ± 0.05[34] | 3.39 |
1727+502 | I Zw 187 | 0.0554 | BL | 7.86[2] | − | LEG | 1.062 | 153359 | 5[37] | 0.80 ± 0.15[34] | – |
1957+405 | Cygnus A | 0.0561 | RG | 9.40[11] | 1.1e−3[20] | HEG | 1.074 | 4491 | 75[38] | 0.55 ± 0.07[38] | ∼5 |
1845+797 | 3C 390.3 | 0.0561 | RG | 8.46[8] | 3.4e−3[18] | HEG | 1.075 | 39025 | 26[39] | 1.71 ± 0.26[34] | – |
0321+340 | 1H 0323+342 | 0.0610 | NLSy1 | 7.30[12] | 2.6e−2[21] | HEG | 1.162 | 607436 | 5[40] | 0.58 ± 0.02[40] | ∼7 |
1219+285 | W Comae | 0.1020 | BL | 8.00[13] | − | LEG | 1.855 | 193940 | 3[41] | 1.28 ± 0.10[34] | – |
1215+303 | ON 325 | 0.1300 | BL | 8.12[2] | − | LEG | 2.291 | 181458 | 2[42] | 1.86 ± 0.40[34] | – |
0806+524 | 1ES 0806+524 | 0.1380 | BL | 8.90[2] | − | LEG | 2.411 | 31747 | 4[37] | 1.32 ± 0.42[34] | – |
1055+567 | 7C 1055+5644 | 0.1433 | BL | 8.54[14] | − | LEG | 2.489 | 74993 | 5[43] | 1.68 ± 0.18[34] | – |
Notes. Column 1: Source name (B1950). Column 2: Other name. Column 3: Redshift. Column 4: Source classification. RG: Radio galaxy, BL: BL Lac, NLSy1: Narrow-line Seyfert 1. Column 5: Log of the black hole mass MBH, expressed in units of solar masses. Column 6: Ratio between the X-ray luminosity in the 2−10 KeV band (reference in the table note) and the Eddington luminosity LEdd = 1.3 × 1038MBH/M⊙. Column 7: Classification as HEG: High-excitation galaxy or LEG: Low-excitation galaxy. A dividing limit LX/LEdd = 1.1e − 3 was assumed. Column 8: Conversion factor, parsec per milliarcsecond. Column 9: Conversion factor, Schwarzschild radii per milliarcsecond. Column 10: Viewing angle. Column 11: Power-law index defining the inner jet shape. Column 12: Transition distance in units of projected milli-arcseconds. References as in Column 11.
References. Column 5: [1] Event Horizon Telescope Collaboration (2019), [2] Woo & Urry (2002), [3] Ferrarese et al. (1996), [4] Satyapal et al. (2005), [5] Aleksić et al. (2014), [6] Balmaverde et al. (2008), [7] Marconi & Hunt (2003), [8] Peterson et al. (2004), [9] Chatterjee et al. (2011), [10] Sikora et al. (2007), [11] Tadhunter et al. (2003), [12] Landt et al. (2017), [13] Xie et al. (2004), [14] Chen et al. (2015). References for the X-ray luminosity used in Column 6: [15] Torresi et al. (2018), [16] Bianchi et al. (2019), [17] González-Martín et al. (2009), [18] Grandi et al. (2006), [19] Gallo et al. (2006), [20] Young et al. (2002), [21] Berton et al. (2019). Columns 10–12 (same as 11) [22] Mertens et al. (2016), [23] Pushkarev et al. (2017), [24] Piner et al. (2001), [25] Canvin et al. (2005), [26] Giovannini et al. (2018), [27] Aleksić et al. (2014) infer an angle range of 10° −20°, we assume the average value, [28] Boccardi et al. (2019), [29] Tseng et al. (2016), [30] Fukazawa et al. (2015), [31] Lico et al. (2012), [32] Giroletti et al. (2004a), [33] MAGIC Collaboration (2020), [34] Kovalev et al. (2020), [35] Sorcia et al. (2013), [36] Giroletti et al. (2006), [37] Costamante & Ghisellini (2002), [38] Boccardi et al. (2016a), [39] Eracleous & Halpern (1994), [40] Hada et al. (2018), [41] Sorcia et al. (2014), [42] Valverde et al. (2020), [43] Ghisellini et al. (2010), [44] Nokhrina et al. (2019), [45] Nakahara et al. (2018).
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