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Table 1.

Physical properties of z > 6 QSOs with new or archival X-ray observations.

ID RA Dec z M1450 Å (m1450 Å) λEdd Ref. (disc./z/MBH) R
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10)
New targets

CFHQS J0050+3445 00:50:06.67 +34:45:21.65 6.253 (Mg II) −26.70 (20.11) 13.45 9.41 0.34 W10/W10/W10 < 11.4
VIK J0109−3047 01:09:53.13 −30:47:26.31 6.7909 ([C II]) −25.64 (21.30) 13.06 9.12 0.27 V13/V16/M17 < 34.1
PSO J036+03 02:26:01.87 +03:02:59.42 6.541 ([C II]) −27.33 (19.55) 13.67 9.48 0.48 V15/B15/M17 < 2.1
VIK J0305−3150 03:05:16.92 −31:50:55.9 6.6145 ([C II]) −26.18 (20.72) 13.26 8.95 0.63 V13/V16/M17 < 20.0
SDSS J0842+1218 08:42:29.43 +12:18:50.58 6.0763 ([C II]) (a) −26.91 (19.86) (a) 13.52 9.29 0.53 dR11/D18/dR11 ( * ), (a) < 1.3
PSO J167−13 11:10:33.98 −13:29:45.60 6.5148 ([C II]) (b) −25.57 (21.25) 13.03 8.48 1.11 V15/M17/M17 < 34.3
CFHQS J1509−1749 15:09:41.78 −17:49:26.80 6.1225 ([C II]) (a) −27.14 (19.64) (a) 13.61 9.47 0.42 W07/D18/W10 (a) < 1.2
CFHQS J1641+3755 16:41:21.73 +37:55:20.15 6.047 (Mg II) −25.67 (21.09) 13.07 8.38 1.51 W07/W10/W10 < 10.5
PSO J338+29 22:32:55.14 +29:30:32.31 6.666 ([C II]) −26.14 (20.78) 13.24 9.43 0.20 V15/M17/M17 < 21.0
SDSS J2310+1855 23:10:38.89 +18:55:19.93 6.0031 ([C II]) −27.80 (18.95) 13.85 9.62 0.52 Wa13/Wa13/J16 < 3.9

QSOs with previous X-ray data

SDSS J0100+2802 01:00:13.02 +28:02:25.92 6.3258 ([C II]) −29.14 (17.69) 14.33 10.03 0.62 Wu15/Wa16/Wu15 ( * ) < 1.2
ATLAS J0142−3327 01:42:43.73 −33:27:45.47 6.379 ([C II]) (a) −27.82 (19.02) (a) 13.85 C15/D18/– < 4.2
CFHQS J0210−0456 02:10:13.19 −04:56:20.90 6.4323 ([C II]) −24.53 (22.33) 12.65 7.90 1.76 W10/W13/W10 < 28.1
CFHQS J0216−0455 02:16:27.81 −04:55:34.10 6.01 (Lyα) −22.49 (24.27) 11.91 W09/W09/– < 23.1
SDSS J0303−0019 03:03:31.40 −00:19:12.90 6.078 (Mg II) −25.56 (21.21) 13.03 8.61 0.81 J08/K09/dR11 ( * ) < 11.4
SDSS J1030+0524 10:30:27.11 +05:24:55.06 6.308 (Mg II) −26.99 (19.84) 13.55 9.21 0.68 F01/K07/dR11 ( * ) < 1.5
SDSS J1048+4637 (c) 10:48:45.07 +46:37:18.55 6.2284 (CO 6-5) −27.24 (19.57) 13.64 9.55 0.38 F03/Wa10/dR11 ( * ) < 0.5
ULAS J1120+0641 11:20:01.48 +06:41:24.30 7.0842 ([C II]) −26.63 (20.38) 13.42 9.39 0.33 M11/V12/M17 < 0.7
SDSS J1148+5251 11:48:16.65 52:51:50.39 6.4189 (CO 6-5) −27.62 (19.24) 13.78 9.71 0.36 F03/Wa11/dR11 ( * )
SDSS J1306+0356 13:06:08.27 +03:56:26.36 6.0337 ([C II]) (a) −26.82 (19.94) (a) 13.49 9.30 0.48 F01/D18/dR11 ( * ), (a) < 1.5
ULAS J1342+0928 13:42:08.27 +09:28:38.61 7.5413 ([C II]) −26.76 (20.34) 13.47 8.89 1.14 B18a/V17/B18a < 4.7
SDSS J1602+4228 16:02:53.98 +42:28:24.94 6.09 (Lyα) −26.94 (19.83) 13.53 F04/F04/–
SDSS J1623+3112 16:23:31.81 +31:12:00.53 6.26 ([C II]) −26.55 (20.27) 13.39 9.15 0.54 F04/Wa11/dR11 ( * ) < 2.3
SDSS J1630+4012 16:30:33.90 +40:12:09.69 6.065 (Mg II) −26.19 (20.58) 13.26 8.96 0.62 F03/I04/dR11 ( * ) < 2.2
HSC J2216−0016 (c) 22:16:44.47 −00:16:50.10 6.10 (Lyα) −23.62 (23.16) 12.32 M16/M16/– < 40.9

Notes. (1): QSO ID. (2) and (3): RA and Dec (J2000) from Bañados et al. (2016, 2018a). (4): Redshift and emission line from which it is derived. In cases of different values derived from different emission lines for the same source, we preferred the redshift derived from the [C II] line rather than the Mg II line, as discussed in Sect. 2.3. (5): Absolute and apparent magnitude at 1450 Å. M1450 Å can vary by up to ≈0.3 mag among different papers, depending on the prescription used to compute it (e.g., Omont et al. 2013 vs. Bañados et al. 2016 for CFHQS J1641+3755). We consistently assumed the values reported by Bañados et al. (2016) and Mazzucchelli et al. (2017), which used the same prescription, for all our sources. (6): Bolometric luminosity estimated from M1450 Å, using the bolometric correction of Venemans et al. (2016). (7): Virial black-hole mass estimated from the Mg II emission line. We note that Trakhtenbrot et al. (2017b) used different calibrations for the black-hole masses of several QSOs included in our sample, typically resulting in larger values (up to ≈0.2 − 0.3 dex). (8): Eddington ratio: λEdd = Lbol/LEdd. (10): Radio-loudness parameter (see Sect. 2.3)

( * )For these QSOs, black-hole masses have been modified according to the Vestergaard & Osmer (2009) calibration, to be consistent with the other QSOs. In these cases, the references indicate the papers from which FWHM(Mg II) and L3000 Å are collected.

(a)

For these sources we updated magnitudes and black-hole masses according to the new [C II]-based redshifts provided by Decarli et al. (2018). These values differ negligibly from those derived assuming previous redshifts based on Mg II or Lyα emission lines.

(b)

Willott et al. (2017) independently reported a slightly different value (z = 6.5157) from [C II].

(c)

Broad absorption-line QSOs (see Fan et al. 2004; Matsuoka et al. 2016).

References. For the QSO discovery, adopted redshift, and black-hole mass. B15: Bañados et al. (2015a); B18a: Bañados et al. (2018a); C15: Carnall et al. (2015); dR11: De Rosa et al. (2011); D18: Decarli et al. (2018); F01: Fan et al. (2001); F03: Fan et al. (2003); F04: Fan et al. (2004); I04: Iwamuro et al. (2004); J08: Jiang et al. (2008); J16: Jiang et al. (2016); K07: Kurk et al. (2007); K09: Kurk et al. (2009); M11: Mortlock et al. (2011); M16: Matsuoka et al. (2016); M17: Mazzucchelli et al. (2017); V12: Venemans et al. (2012); V13: Venemans et al. (2013); V15: Venemans et al. (2015); V16: Venemans et al. (2016); V17: Venemans et al. (2017); W07: Willott et al. (2007); W09: Willott et al. (2009); W10: Willott et al. (2010); W13: Willott et al. (2013); Wa10: Wang et al. (2010); Wa11: Wang et al. (2011); Wa13: Wang et al. (2013); Wa16: Wang et al. (2016); Wu15: Wu et al. (2015).

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