2023A&A...669A..83D


Query : 2023A&A...669A..83D

2023A&A...669A..83D - Astronomy and Astrophysics, volume 669A83 (2023/1-1)

High-redshift quasars along the main sequence.

DECONTO-MACHADO A., DEL OLMO OROZCO A., MARZIANI P., PEREA J. and STIRPE G.M.

Abstract (from CDS):


Context. The 4D Eigenvector 1 empirical formalism (4DE1) and its main sequence (MS) for quasars has emerged as a powerful tool for organising the diversity among quasar populations, as several key observational measures and physical parameters are systematically changing along it.
Aims. Trends revealed by 4DE1 are very well established to explain all the diverse characteristics seen in low-redshift quasar samples. Nevertheless, the situation is far less clear when dealing with high-luminosity and high-redshift sources. Here, we aim to evaluate the behaviour of our sample of 22 quasars at high redshift (2.2 ≤ z ≤ 3.7) and high luminosity (47.39 ≤ Lbol ≤ 48.36) in the context of the 4DE1.
Methods. Our approach involves studying quasar physics through a spectroscopic exploration of UV and optical emission line diagnostics. We used new observations from the ISAAC instrument at ESO-VLT and primarily from the SDSS to cover the optical and the UV rest-frames, respectively. The emission lines were characterised both via a quantitative parametrisation of the line profiles and a decomposition of the emission line profiles using multicomponent fitting routines.
Results. We provide spectrophotometric properties and line profile measurements for Hβ+[O III]λλ4959,5007, as well as Si IVλ1397+O IV]λ1402, C IVλ1549+He IIλ1640, and the 1900 Å blend (including Al IIIλ1860, Si III]λ1892, and C III]λ1909). For six out of the 22 objects, a significantly blueshifted component on the Hβ profile is present. In 14 out of 22 cases, an Hβ outflowing component associated with [O III] is detected. The majority of [O III]λλ4959,5007 emission line profiles show blueshifted velocities higher than 250 km s–1. We find extremely broad [O III]λλ4959,5007 emission that is comparable to the width of Hβ broad profile in some highly accreting quasars. The [O III]λλ4959,5007 and C IVλ1549 blueshifts show very high amplitudes and a high degree of correlation. The line widths and shifts are correlated for both [O III]λλ4959,5007 and C IVλ1549, suggesting that emission from outflowing gas is providing a substantial broadening effect to both lines. Otherwise, the links between C IVλ1549 centroid velocity at half intensity (c(1/2)), Eddington ratio (L/LEdd), and bolometric luminosity are found to be in agreement with previous studies of high-luminosity quasars.
Conclusions. Our analysis suggests that the behaviour of quasars of very high luminosity all along the main sequence is strongly affected by powerful outflows involving a broad range of spatial scales. The main sequence correlations remain valid at high redshift and high luminosity even if a systematic increase in line width is observed. Scaling laws based on UV Al IIIλ1860 and Hβ emission lines are equally reliable estimators of MBH.

Abstract Copyright: © The Authors 2023

Journal keyword(s): quasars: general - quasars: emission lines - quasars: supermassive black holes

VizieR on-line data: <Available at CDS (J/A+A/669/A83): table1.dat sp/*>

Simbad objects: 24

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Number of rows : 24
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 QSO J0003-2323 QSO 00 03 44.9144535192 -23 23 55.073021280     16.7     ~ 79 0
2 [VV2006] J002830.5-281706 QSO 00 28 30.4642386648 -28 17 05.238885732     18.01     ~ 27 0
3 QSO B0029+073 QSO 00 32 18.3629227824 +07 38 32.567030700     18.4     ~ 40 0
4 QSO J0041-4936 QSO 00 41 31.4401078248 -49 36 11.686921488   17.9 17.9     ~ 26 0
5 [VV2006] J005700.2+143738 QSO 00 57 00.1917547800 +14 37 37.787199636   18.28 17.96     ~ 32 0
6 QSO B0055-26 QSO 00 57 58.0253990928 -26 43 14.750912928   17.90 17.47 17.99   ~ 152 1
7 QSO B0940-1050 QSO 09 42 53.5078384704 -11 04 25.931336376   16.96 16.6 16.6   ~ 102 0
8 [VV2006] J114358.6+052445 QSO 11 43 58.5246314448 +05 24 45.055975392   17.55 17.27     ~ 35 0
9 2MASS J11595433+2019212 QSO 11 59 54.3311536560 +20 19 21.135293688   18.55 17.92     ~ 29 0
10 QSO B1159+123 QSO 12 01 47.9118521640 +12 06 30.253926276   18.85 18.16     ~ 108 0
11 2MASS J13201235+1420370 QSO 13 20 12.3437239848 +14 20 37.090680720   17.97 17.82     ~ 19 0
12 [VV2006] J135831.8+050522 QSO 13 58 31.7861805216 +05 05 22.766861292   17.57 17.33     ~ 36 0
13 QSO B1410+0936 QSO 14 13 21.0603550608 +09 22 04.849158468     17.8     ~ 41 0
14 QSO J1415+1129 QSO 14 15 46.25 +11 29 43.4   17.63 17.23     ~ 678 0
15 QSO B1422+2309 BLL 14 24 38.0938 +22 56 00.587   16.77 15.84 14.79   ~ 464 1
16 QSO J1538+0855 QSO 15 38 30.5596599072 +08 55 17.150004552   18.77 17.98     ~ 39 0
17 SDSS J161458.33+144837.0 QSO 16 14 58.3387483752 +14 48 36.948344148   17.62 17.43     ~ 26 0
18 QSO B1937-1009 BLL 19 39 57.2566747152 -10 02 41.522299692   18.800 19.0 17.188   ~ 207 1
19 QSO B2000-330 Bla 20 03 24.1161711720 -32 51 45.136882080   18.83 18.4 17.11   ~ 279 1
20 2MASS J21052449+0004073 QSO 21 05 24.4929889752 +00 04 07.267776384   17.56 16.98     ~ 17 0
21 [VV2006] J210831.6-063022 QSO 21 08 31.5672867288 -06 30 22.582588536   17.71 17.41     ~ 36 0
22 SDSS J212329.46-005052.9 QSO 21 23 29.4639412848 -00 50 52.916363736   16.91 16.62     ~ 131 0
23 QSO B2126-15 Bla 21 29 12.17589329 -15 38 41.0419083   17.61 17.3 17.3   ~ 521 1
24 QSO B2355+01 QSO 23 58 08.5422487128 +01 25 07.227052428   17.5 17.5     ~ 28 0

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