2023A&A...677A.111T


Query : 2023A&A...677A.111T

2023A&A...677A.111T - Astronomy and Astrophysics, volume 677A111 (2023/9-1)

The most luminous blue quasars at 3.0 < z < 3.3 III. LBT spectra and accretion parameters.

TREFOLONI B., LUSSO E., NARDINI E., RISALITI G., BARGIACCHI G., BISOGNI S., CIVANO F.M., ELVIS M., FABBIANO G., GILLI R., MARCONI A., RICHARDS G.T., SACCHI A., SALVESTRINI F., SIGNORINI M. and VIGNALI C.

Abstract (from CDS):

We present the analysis of the rest frame ultraviolet and optical spectra of 30 bright blue quasars at z ∼ 3, selected to examine the suitability of active galactic nuclei as cosmological probes. In our previous works, based on pointed XMM-Newton observations, we found an unexpectedly high fraction (≈25%) of X-ray weak quasars in the sample. The latter sources also display a flatter UV continuum and a broader and fainter C IV profile in the archival UV data with respect to their X-ray normal counterparts. Here we present new observations with the Large Binocular Telescope in both the zJ (covering the rest frame ≃2300-3100 Å) and the KS (≃4750-5350 Å) bands. We estimated black hole masses (MBH) and Eddington ratios (λEdd) from the available rest frame optical and UV emission lines (Hβ, Mg II), finding that our z ∼ 3 quasars are on average highly accreting (⟨λEdd⟩≃1.2 and ⟨MBH⟩≃109.7 M⊙), with no difference in λEdd or MBH between X-ray weak and X-ray normal quasars. From the zJ spectra, we derived the properties (e.g. flux, equivalent width) of the main emission lines (Mg II, Fe II), finding that X-ray weak quasars display higher Fe II/Mg II ratios with respect to typical quasars. Fe II/Mg II ratios of X-ray normal quasars are instead consistent with other estimates up to z ≃ 6.5, corroborating the idea of already chemically mature broad line regions at early cosmic time. From the KS spectra, we find that all the X-ray weak quasars present generally weaker [O III] emission (EW < 10 Å) than the normal ones. The sample as a whole, however, abides by the known X-ray-[O III] luminosity correlation, hence the different [O III] properties are likely due to an intrinsically weaker [O III] emission in X-ray weak objects, associated to the shape of the spectral energy distribution. We interpret these results in the framework of accretion-disc winds.

Abstract Copyright: © The Authors 2023

Journal keyword(s): galaxies: active - quasars: general - quasars: supermassive black holes - quasars: emission lines - accretion - accretion disks

Simbad objects: 31

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Number of rows : 31
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 LBQS 0301-0035 QSO 03 03 41.0487601176 -00 23 21.907819248   18.26 17.93 17.6   ~ 121 0
2 LBQS 0302-0019 QSO 03 04 49.8593341368 -00 08 13.534398816   18.08 17.80 17.5   ~ 261 0
3 QSO J0826+3148 QSO 08 26 19.7049044064 +31 48 48.019135932   18.29 17.99     ~ 49 0
4 2MASS J08353569+2122401 QSO 08 35 35.6917373592 +21 22 40.224996840   18.73 18.36     ~ 32 0
5 QSO B0900+42 QSO 09 00 33.5091652824 +42 15 47.031009948   17.63 17.18     ~ 85 0
6 [VV2006] J090103.0+354928 QSO 09 01 02.9371522872 +35 49 28.546792536   18.30 18.00     ~ 38 0
7 [VV2006] J090508.8+305756 QSO 09 05 08.8856022480 +30 57 57.274061004   18.02 17.78     ~ 33 0
8 QSO J0942+0422 QSO 09 42 02.0480819568 +04 22 44.548204368   17.78 17.47     ~ 66 0
9 2MASS J09455500+2305384 QSO 09 45 54.9952004328 +23 05 38.682354228   19.38 18.92     ~ 20 0
10 2MASS J09473420+1421168 QSO 09 47 34.1970129912 +14 21 16.944191676   17.89 17.65     ~ 39 0
11 QSO B1011+4315 QSO 10 14 47.1891688176 +43 00 30.167514324   17.39 17.05     ~ 74 0
12 [VV2000] J102714.7+354318 QSO 10 27 14.7800880984 +35 43 17.395124844   16.96 16.69     ~ 50 0
13 2MASS J11110130-1505183 QSO 11 11 01.3020327600 -15 05 18.519922896           ~ 16 0
14 2MASS J11112059+2437408 QSO 11 11 20.5860582552 +24 37 40.886982912   18.34 17.97     ~ 25 0
15 QSO J1143+3452 QSO 11 43 08.8809241248 +34 52 22.233156204   17.43 17.15     ~ 49 0
16 [VV2000] J114851.4+231340 QSO 11 48 51.4730628120 +23 13 40.438137576   18.77 18.29     ~ 26 0
17 2MASS J11591153+3134272 QSO 11 59 11.5313895000 +31 34 27.240076992   18.40 18.11     ~ 36 0
18 QSO J1201+0116 QSO 12 01 44.3649782736 +01 16 11.740001304   18.09 17.74 17.4   ~ 66 2
19 [VV2006] J122017.0+454941 QSO 12 20 17.0720096088 +45 49 41.104511544   19.39 18.85     ~ 30 0
20 QSO J1225+4831 QSO 12 25 18.66000 +48 31 16.3020   18.69 18.30     ~ 41 0
21 2MASS J12463704+2625005 QSO 12 46 37.0609409328 +26 25 00.309738432   18.18 17.83     ~ 24 0
22 LBQS 1244+1129 QSO 12 46 40.3700829816 +11 13 02.901704808     18.4     ~ 64 0
23 [VV2006] J140747.2+645420 QSO 14 07 47.2332082608 +64 54 19.916965836   17.73 17.41     ~ 43 0
24 [VV2006] J142543.3+540619 QSO 14 25 43.3298905704 +54 06 19.327380048   18.64 18.22     ~ 46 0
25 QSO B1425+606 QSO 14 26 56.1849081360 +60 25 50.813373324   16.82 16.54     ~ 148 0
26 QSO J1459+0024 QSO 14 59 07.1942637720 +00 24 01.272819600   19.43 18.87     ~ 46 0
27 SDSS J150731.48+241910.8 QSO 15 07 31.4873309664 +24 19 10.782769152   19.93 19.60     ~ 19 0
28 [VV2006] J153201.6+370002 QSO 15 32 01.5985744128 +37 00 02.333276064   18.12 17.80     ~ 35 0
29 QSO J1712+5755 QSO 17 12 27.7465195944 +57 55 06.895257456   17.75 17.53     ~ 45 0
30 PHL 1811 Sy1 21 55 01.5124437432 -09 22 24.349496808   13.9 16.8 14.1   ~ 200 1
31 LBQS 2230-0015 QSO 22 34 08.9971751592 +00 00 01.703853180   18.09 17.39 17.3   ~ 142 0

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