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Table B.1.

Emission properties of Mg II and C IV, along with the derived quasar physical quantities: redshift, lines FWHM, C IV blueshift, C IV–Mg II velocity shift, monochromatic luminosity at 3000Å, bolometric luminosity, black hole mass, and Eddington ratio.

Quasar zMg II FWHMC IV FWHMMg II C IV blueshift Δv(C IV-Mg II) log λL3000Å log Lbol log MBH,C IV log MBH,Mg IV λEdd,C IV λEdd,C II
[km/s] [km/s] [km/s] [km/s] [erg s−1] [erg s−1] [M] [M]
J0251+0333* 4.9900 ± 0.0008 4430 ± 130 2590 ± 60 1250 ± 60 −410 ± 40 46.79 ± 0.05 47.50 ± 0.05 9.35 ± 0.04 9.08 ± 0.03 1.1 ± 0.2 2.0 ± 0.3
J2344+1653* 4.9980 ± 0.0003 6850 ± 860 3530 ± 240 −230 ± 140 −350 ± 200 47.04 ± 0.12 47.75 ± 0.12 10.47 ± 0.14 9.47 ± 0.08 0.1 ± 0.1 1.4 ± 0.5
J1200+1817* 5.0000 ± 0.0010 5970 ± 90 2960 ± 110 1720 ± 40 −1460 ± 50 46.60 ± 0.13 47.32 ± 0.13 9.43 ± 0.07 9.10 ± 0.07 0.6 ± 0.2 1.2 ± 0.4
J0221-0342* 5.0170 ± 0.0008 2750 ± 230 2200 ± 80 1050 ± 60 −370 ± 80 46.73 ± 0.11 47.44 ± 0.11 8.94 ± 0.36 8.91 ± 0.06 2.4 ± 2.1 2.6 ± 0.8
J0017-1000* 5.0170 ± 0.0020 5810 ± 100 3420 ± 210 2330 ± 60 −2070 ± 100 46.63 ± 0.10 47.35 ± 0.10 9.24 ± 0.03 9.24 ± 0.07 0.6 ± 1.1 1.0 ± 0.3
J0846+0800* 5.0210 ± 0.0016 8680 ± 190 3110 ± 130 3400 ± 100 −3140 ± 90 46.52 ± 0.14 47.23 ± 0.14 9.37 ± 0.82 9.10 ± 0.08 1.0 ± 0.2 1.0 ± 0.4
J0338+0021* 5.0230 ± 0.0005 7200 ± 1830 3510 ± 270 3280 ± 1010 −1560 ± 1720 46.44 ± 0.22 47.15 ± 0.22 9.22 ± 0.30 9.17 ± 0.13 0.7 ± 0.6 0.7 ± 0.4
J1423+1303* 5.0462 ± 0.0018 7590 ± 100 4030 ± 270 2330 ± 40 −2070 ± 80 46.68 ± 0.15 47.39 ± 0.15 9.54 ± 0.02 9.41 ± 0.09 10.1 ± 6.0 0.7 ± 0.3
J1601-1828* 5.0502 ± 0.0006 6180 ± 580 3560 ± 140 4210 ± 310 −2760 ± 270 46.70 ± 0.04 47.41 ± 0.04 8.96 ± 0.11 9.31 ± 0.04 0.5 ± 0.2 1.0 ± 0.1
J0025-0145* 5.0630 ± 0.0030 5500 ± 1480 2310 ± 40 8080 ± 920 −920 ± 0 47.19 ± 0.07 47.90 ± 0.07 8.78 ± 0.25 9.18 ± 0.04 0.8 ± 0.6 4.0 ± 0.7
J1004+2025* 5.0634 ± 0.0014 14830 ± 1880 5450 ± 350 5030 ± 250 −3160 ± 320 46.53 ± 0.24 47.24 ± 0.24 9.57 ± 0.27 9.60 ± 0.13 2.2 ± 0.6 0.3 ± 0.2
J0835+0537 5.0643 ± 0.0010 7130 ± 150 3590 ± 130 4210 ± 110 −4000 ± 120 46.47 ± 0.14 47.18 ± 0.14 9.02 ± 0.03 9.20 ± 0.08 1.1 ± 0.4 0.7 ± 0.3
J2202+1509 5.0755 ± 0.0007 5550 ± 290 4370 ± 620 1630 ± 80 −1380 ± 220 46.91 ± 0.33 47.62 ± 0.33 9.60 ± 0.05 9.60 ± 0.20 0.4 ± 0.3 0.8 ± 0.7
J0115-0253* 5.0820 ± 0.0020 5900 ± 320 4720 ± 80 2210 ± 90 −2050 ± 100 46.49 ± 0.19 47.20 ± 0.19 9.27 ± 0.08 9.45 ± 0.10 0.7 ± 0.3 0.4 ± 0.2
J2201+0302* 5.0887 ± 0.0025 6360 ± 200 4250 ± 200 3280 ± 70 −2280 ± 90 46.71 ± 0.19 47.42 ± 0.19 9.25 ± 0.03 9.47 ± 0.10 1.8 ± 0.9 0.7 ± 0.3
J2226-0618* 5.1050 ± 0.0010 5630 ± 1090 3460 ± 220 2380 ± 270 −1600 ± 310 47.07 ± 0.10 47.78 ± 0.10 9.40 ± 0.18 9.47 ± 0.07 1.1 ± 0.5 1.6 ± 0.4
J0957+1016* 5.1274 ± 0.0011 7750 ± 180 4890 ± 750 2620 ± 90 −2350 ± 240 46.37 ± 0.14 47.08 ± 0.14 9.37 ± 0.09 9.42 ± 0.15 0.4 ± 0.2 0.3 ± 0.2
J0957+0610* 5.1650 ± 0.0030 7210 ± 200 4190 ± 430 2090 ± 80 −1890 ± 180 46.76 ± 0.14 47.47 ± 0.14 9.58 ± 0.03 9.48 ± 0.12 0.6 ± 0.2 0.7 ± 0.3
J0854+2056* 5.1715 ± 0.0007 2210 ± 100 2450 ± 540 790 ± 20 20 ± 70 46.69 ± 0.12 47.40 ± 0.12 8.84 ± 0.04 8.98 ± 0.20 2.8 ± 0.9 2.0 ± 1.1
J0241+0435* 5.1900 ± 0.0006 4080 ± 380 3260 ± 140 1160 ± 70 −540 ± 80 46.65 ± 0.12 47.36 ± 0.12 9.25 ± 1.48 9.21 ± 0.07 1.0 ± 0.2 1.1 ± 0.4
J0131-0321* 5.1942 ± 0.0007 6400 ± 450 2750 ± 70 1400 ± 160 −830 ± 160 47.32 ± 0.07 48.04 ± 0.07 9.92 ± 0.08 9.40 ± 0.04 1.0 ± 3.4 3.3 ± 0.6
J0902+0851* 5.2200 ± 0.0008 2520 ± 110 2070 ± 220 470 ± 30 −20 ± 50 46.40 ± 0.19 47.11 ± 0.19 8.97 ± 0.05 8.69 ± 0.13 1.1 ± 0.5 2.0 ± 1.1
J0216+2304* 5.2273 ± 0.0005 5960 ± 690 3930 ± 190 2700 ± 220 −1720 ± 240 46.67 ± 0.12 47.39 ± 0.12 9.20 ± 0.13 9.39 ± 0.07 0.8 ± 0.7 0.8 ± 0.3
J2325-0553* 5.2304 ± 0.0005 7170 ± 2290 4870 ± 400 2700 ± 560 −1570 ± 1800 46.76 ± 0.19 47.47 ± 0.19 9.45 ± 0.30 9.61 ± 0.12 1.2 ± 0.5 0.6 ± 0.3
J1436+2132* 5.2356 ± 0.0005 5500 ± 970 3420 ± 110 1830 ± 210 −870 ± 600 46.45 ± 0.26 47.16 ± 0.26 9.30 ± 0.17 9.15 ± 0.13 1.0 ± 0.1 0.8 ± 0.5
J2351-0459* 5.2481 ± 0.0009 5180 ± 850 3780 ± 120 1400 ± 270 −680 ± 270 46.46 ± 0.17 47.17 ± 0.17 9.34 ± 0.27 9.24 ± 0.09 0.5 ± 0.4 0.7 ± 0.3
J2225+0330* 5.2523 ± 0.0004 4780 ± 560 5450 ± 100 1600 ± 250 −740 ± 110 46.49 ± 0.18 47.20 ± 0.18 9.17 ± 0.12 9.58 ± 0.09 0.6 ± 0.4 0.3 ± 0.1
J1147-0109* 5.2544 ± 0.0006 9070 ± 210 5680 ± 260 1150 ± 90 −890 ± 100 46.77 ± 0.28 47.48 ± 0.28 10.04 ± 0.04 9.75 ± 0.15 0.8 ± 0.4 0.4 ± 0.3
J0747+1153 5.2575 ± 0.0004 5050 ± 140 3040 ± 60 1050 ± 20 −840 ± 30 47.19 ± 0.03 47.90 ± 0.03 9.77 ± 0.03 9.42 ± 0.02 0.2 ± 0.1 2.3 ± 0.2
J2330+0957 5.2889 ± 0.0007 11390 ± 2840 4260 ± 420 3140 ± 680 −3010 ± 630 46.61 ± 0.12 47.32 ± 0.12 9.64 ± 1.04 9.43 ± 0.10 1.0 ± 0.6 0.6 ± 0.2
J2358+0634 5.2973 ± 0.0007 7200 ± 960 3360 ± 380 3570 ± 250 −2660 ± 350 46.70 ± 0.23 47.41 ± 0.23 9.28 ± 0.12 9.26 ± 0.15 0.4 ± 0.9 1.1 ± 0.7
J0812+0440 5.3026 ± 0.0009 3000 ± 70 2400 ± 60 670 ± 20 −180 ± 30 46.58 ± 0.09 47.30 ± 0.09 9.12 ± 0.03 8.91 ± 0.05 1.1 ± 0.2 1.9 ± 0.4
J0116+0538 5.3310 ± 0.0004 6290 ± 540 3910 ± 190 2330 ± 120 −1880 ± 250 46.74 ± 0.24 47.45 ± 0.24 9.42 ± 0.08 9.41 ± 0.13 0.8 ± 0.5 0.8 ± 0.5
J0155+0415 5.3596 ± 0.0011 8890 ± 1730 4340 ± 390 4590 ± 540 −3480 ± 770 46.70 ± 0.21 47.41 ± 0.21 9.28 ± 0.19 9.48 ± 0.13 1.0 ± 0.7 0.6 ± 0.4
J0306+1853 5.3649 ± 0.0005 7850 ± 350 5690 ± 1330 2790 ± 130 −2460 ± 1490 47.52 ± 0.25 48.23 ± 0.25 9.92 ± 0.05 10.13 ± 0.24 1.6 ± 0.9 1.0 ± 0.8
J1022+2252(a) 5.47 ± 0.01(b) 3410 ± 340 1130 ± 100 46.80 ± 0.09 47.51 ± 0.09 9.18 ± 0.09 1.7 ± 0.5
J2207-0416(a) 5.523 ± 0.004 6300 ± 1210 4070 ± 240 1250 ± 330 −990 ± 270 47.10 ± 0.06 47.81 ± 0.06 9.74 ± 0.19 9.63 ± 0.06 0.9 ± 0.4 1.2 ± 0.2
J0108+0711(a) 5.5578 ± 0.0018 5040 ± 460 2770 ± 1120 2590 ± 170 −2320 ± 260 46.74 ± 0.14 47.45 ± 0.14 9.18 ± 0.09 9.11 ± 0.36 1.5 ± 0.6 1.7 ± 1.5
J1335-0328(a) 5.699 ± 0.001(b) 4650 ± 120 2090 ± 60 46.83 ± 0.21 47.55 ± 0.21 9.34 ± 0.03 1.2 ± 0.6

Notes: Quasars marked with an asterisk are in common with the XQz5 sample described in Lai et al. (2024). The reported errors account only for the statistical uncertainties. Black hole masses and bolometric luminosities are also affected by systematic uncertainties of 0.5 dex and 0.3 dex, respectively. (a) Mg II emission line contaminated by telluric emission. (b) Redshift estimated from the apparent start of the Lyα forest (Becker et al. 2019). (c) Redshift estimated from the [C II] emission line (Table 5).

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