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Table 5.

Properties of MgIIλ2800 emission line derived from parametric model fits (see Sect. 3.2).

ID FWHMMgII EWMgII Log (LMgII/erg s−1) Log (L3000/erg s−1)
(Å) (km s−1) (Å) (km s−1)
X_N_160_22 2804 ± 1 3620 ± 180 25 ± 1 −390 ± 80 44.45 ± 0.07 46.46 ± 0.06
X_N_81_44 2801 ± 1 3910 ± 250 36 ± 2 −90 ± 100 44.37 ± 0.07 46.25 ± 0.06
X_N_53_3 2795 ± 1 2880 ± 290 17 ± 2 530 ± 120 44.18 ± 0.08 46.32 ± 0.06
X_N_66_23 2795 ± 3 3180 ± 880 26 ± 8 510 ± 340 43.70 ± 0.13 45.78 ± 0.07
X_N_4_48 2790 ± 4 8730 ± 1040 83 ± 14 1030 ± 380 44.27 ± 0.09 45.70 ± 0.07
X_N_102_35 2800 ± 1 4110 ± 190 23 ± 1 −2 ± 80 44.33 ± 0.07 46.40 ± 0.06
X_N_115_23 2803 ± 2 4320 ± 550 56 ± 8 −360 ± 210 44.12 ± 0.09 45.82 ± 0.07
cid_166 2803 ± 1 5910 ± 340 35 ± 2 −270 ± 140 44.64 ± 0.07 46.49 ± 0.06
cid_1605 2801 ± 1 4210 ± 420 42 ± 5 −150 ± 160 43.77 ± 0.08 45.50 ± 0.07
cid_346 2802 ± 2 5400 ± 660 29 ± 4 −220 ±250 44.03 ± 0.08 45.99 ± 0.06
cid_467 2801 ± 5 5830 ± 1340 17 ± 4 −60 ± 500 43.77 ± 0.11 45.95 ± 0.06
J1333+1649 2794 ± 1 3690 ± 80 12 ± 0 680 ± 30 45.15 ± 0.07 47.47 ± 0.06
J1441+0454 2792 ± 1 4010 ± 100 20 ± 0 880 ± 40 44.96 ± 0.07 47.05 ± 0.06
J1549+1245 2804 ± 1 3150 ± 70 22 ± 1 −410 ± 30 45.07 ± 0.07 47.15 ± 0.06
S82X1905 2805 ± 3 4430 ± 770 20 ± 4 −530 ± 330 43.93 ± 0.10 45.98 ± 0.06
S82X1940 2788 ± 2 3410 ± 500 370 ± 271 1240 ± 190 43.98 ± 0.09 43.63 ± 0.57
S82X2058 2792 ± 3 4490 ± 630 30 ± 4 910 ± 270 44.09 ± 0.09 46.09 ± 0.06

Notes. Columns give the following information for the BLR component of the MgII emission line: (1) target identification, (2) centroid (Å), (3) FWHM (km s−1), (4) rest-frame EW (Å), (5) velocity of the MgII at 50% of the cumulative line flux, (6) logarithm of the extinction-corrected MgII luminosity, and (7) logarithm of the extinction-corrected luminosity at 3000 Å derived from the best-fit values of the power-law model representing the AGN continuum (see Sect. 3).

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