2020A&A...635A.151B


Query : 2020A&A...635A.151B

2020A&A...635A.151B - Astronomy and Astrophysics, volume 635A151-151 (2020/3-1)

Selection of highly-accreting quasars. Spectral properties of Fe IIopt emitters not belonging to extreme Population A.

BON N., MARZIANI P., BON E., NEGRETE C.A., DULTZIN D., DEL OLMO A., D'ONOFRIO M. and MARTINEZ-ALDAMA M.L.

Abstract (from CDS):


Context. The quasar class of extreme Population A (xA) (also known as super-Eddington accreting massive black holes, SEAMBHs) has been hailed as potential distance indicators for cosmology.
Aims. The aim of this paper is to define tight criteria for their proper identification, starting from the main selection criterion RFeII>1, and to identify potential intruders that do not meet the selection criteria, which nonetheless have been selected as xA because of the coarseness of automatic searches. The inclusion of the spurious xA sources may dramatically increase the dispersion in the Hubble diagram of quasars, which were obtained from virial luminosity estimates.
Methods. We studied a sample of 32 low-z quasars that were originally selected from the seventh data release of the Sloan Digital Sky Survey as xA or SEAMBHs, which have been proved to be almost certainly misclassified sources. All of them show moderate to strong FeII emission and the large majority show strong absorption features in their spectra which are typical of fairly evolved stellar populations. We performed a simultaneous fit of a host galaxy spectrum, active galactic nucleus (AGN) continuum, FeII template, and emission lines to spectra, using the fitting technique based on ULySS, the full spectrum fitting package. We derived the main accretion parameters (i.e., luminosity, black hole mass, and Eddington ratio) and investigate the relation between host galaxy properties and AGN.
Results. For sources in our sample with spectral types that correspond to a relatively low Eddington ratio, we find an overall consistency between HβNC, [OIII]λλ4959,5007 line shifts, and the mean stellar velocity obtained from the host galaxy fit (within ≤|60|km/s). Only one source in our sample qualifies as a xA source.
Conclusions. The correct classification of spectra that were contaminated by heavy absorption requires careful determination of the host galaxy spectrum. Contamination and misclassification are not usual in the identification of the xAs, nor at low z or at high z. We find a high fraction of host galaxy spectrum; in half of the sample this is even higher than 40%. When absorption lines are prominent, and the fraction of the host galaxy is high, host galaxy spectrum mimics FeII, which may result in a mistaken identification of FeII spectral features. We have identified several stellar absorption lines that, along with the continuum shape, may lead to an overestimate of RFeII, and therefore to the misclassification of sources as xA sources.

Abstract Copyright: © ESO 2020

Journal keyword(s): quasars: general - quasars: emission lines - quasars: absorption lines - cosmology: miscellaneous - galaxies: stellar content - quasars: supermassive black holes

Simbad objects: 35

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Number of rows : 35
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 2MASX J00365714-1008102 Sy1 00 36 57.1783879344 -10 08 10.691789136   18.01 17.53 16.91   ~ 25 0
2 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
3 2MASS J01093393+1525591 Sy1 01 09 33.9230723160 +15 25 59.092085460   19.31 18.86     ~ 19 0
4 2MASS J01180797+1505130 Sy1 01 18 07.9835078352 +15 05 12.902602740   19.44 18.93     ~ 19 0
5 2MASS J03171509-0738221 Sy1 03 17 15.1059102936 -07 38 22.325093952   19.45 18.90     ~ 19 0
6 2MASS J07505987+3520052 Sy1 07 50 59.8268866752 +35 20 05.234501256   19.67 19.31     ~ 20 0
7 SDSS J082205.19+584058.3 QSO 08 22 05.1912142296 +58 40 58.289307744   19.97 19.53     ~ 10 0
8 2MASS J08220524+4553493 Sy1 08 22 05.2446852192 +45 53 49.141858452   18.71 18.31     ~ 26 0
9 2MASS J09101704+0602385 QSO 09 10 17.0750210688 +06 02 38.655361572   19.49 18.96     ~ 19 0
10 2MASS J09102008+3124177 Sy1 09 10 20.1108352824 +31 24 17.835329952   18.90 18.49     ~ 16 0
11 Mrk 110 Sy1 09 25 12.8479065576 +52 17 10.386311208   16.82 16.41     ~ 681 1
12 2MASS J09262061+1017349 Sy1 09 26 20.6224301136 +10 17 34.801920348   19.56 19.04     ~ 18 0
13 2MASS J09424940+5932063 Sy1 09 42 49.4045339376 +59 32 06.381838392   19.18 18.66     ~ 22 0
14 2MASS J09430585+5350482 QSO 09 43 05.8881488688 +53 50 48.426147096   19.50 19.02     ~ 21 0
15 2MASS J10302124+1708253 Sy1 10 30 21.2456333040 +17 08 25.370284380   19.09 18.65     ~ 13 0
16 2MASS J10553041+1321179 Sy1 10 55 30.4097330424 +13 21 17.841288744   18.05 17.69     ~ 19 0
17 LEDA 3440428 Sy1 10 57 05.4054483024 +58 04 37.463567088   18.00 17.50 17.27 16.85 ~ 49 0
18 2MASX J11293079+4310174 Sy1 11 29 30.7647418008 +43 10 17.334684336   18.76 18.23     ~ 23 0
19 2MASS J11363013+6219021 Sy1 11 36 30.1058854320 +62 19 02.404408872   19.05 18.53     ~ 25 0
20 LEDA 3582384 Sy2 11 36 51.6670731744 +44 50 16.390473936   18.11 17.56     ~ 28 0
21 NGC 3779 GiG 11 38 51.06 -10 35 01.5   14.42   13.89 14.4 ~ 37 0
22 2MASS J12343107+5156293 Sy1 12 34 31.0826983560 +51 56 29.209949916   19.52 18.96     ~ 24 0
23 2MASS J12453382+5348383 QSO 12 45 33.8739346008 +53 48 38.291315904   18.81 18.42     ~ 20 0
24 2MASS J12521957+1820364 Sy1 12 52 19.5535674840 +18 20 36.021790968   19.36 18.72     ~ 15 1
25 2MASS J13361231+0947467 Sy1 13 36 12.3001595856 +09 47 46.909056300   19.44 18.87     ~ 14 0
26 2MASS J13474807+4046326 Sy1 13 47 48.0701773392 +40 46 32.748048984   19.60 18.96     ~ 18 0
27 2MASS J13493808+0335439 Sy1 13 49 38.0895170616 +03 35 43.931905944   19.09 18.50     ~ 20 0
28 2MASS J13500856+2331461 Sy1 13 50 08.5519621440 +23 31 46.063836912   18.58 18.23     ~ 13 0
29 2MASS J14113186+4420014 Sy1 14 11 31.8644248104 +44 20 00.989746656   19.23 18.64     ~ 22 0
30 2MASS J14365151+3436023 Sy1 14 36 51.5120169624 +34 36 02.446290792   19.58 19.13 17.74 17.08 ~ 26 0
31 2MASS J15160039+5724156 Sy1 15 16 00.3938308008 +57 24 15.674883012   18.59 18.08     ~ 23 0
32 2MASS J15595079+5125043 Sy1 15 59 50.7883701480 +51 25 04.119586464   18.98 18.55     ~ 22 0
33 2MASS J16100270+2021085 Sy1 16 10 02.7042345624 +20 21 08.486354556   19.14 18.55     ~ 16 0
34 2MASS J16261217+1430291 Sy1 16 26 12.1699650072 +14 30 29.076022800   20.19 19.48     ~ 13 0
35 2MASS J17025047+3344097 Sy1 17 02 50.4698479848 +33 44 09.690895428   18.43 17.96     ~ 26 0

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