2019A&A...632A.109N


Query : 2019A&A...632A.109N

2019A&A...632A.109N - Astronomy and Astrophysics, volume 632A109-109 (2019/12-0)

The most luminous blue quasars at 3.0 < z < 3.3. I. A tale of two X-ray populations.

NARDINI E., LUSSO E., RISALITI G., BISOGNI S., CIVANO F., ELVIS M., FABBIANO G., GILLI R., MARCONI A., SALVESTRINI F. and VIGNALI C.

Abstract (from CDS):

We present the X-ray analysis of 30 luminous quasars at z~=3.0-3.3 with pointed XMM-Newton observations (28-48 ks) originally obtained by our group to test the suitability of active galactic nuclei as standard candles for cosmological studies. The sample was selected in the optical from the Sloan Digital Sky Survey Data Release 7 to be representative of the most luminous, intrinsically blue quasar population, and by construction boasts a high degree of homogeneity in terms of optical and UV properties. In the X-rays, only four sources are too faint for a detailed spectral analysis, one of which is formally undetected. Neglecting one more object later found to be radio-loud, the other 25 quasars are, as a whole, the most X-ray luminous ever observed, with rest-frame 2-10keV luminosities of 0.5-7x1045erg/s. The continuum photon index distribution, centred at Γ∼1.85, is in excellent agreement with those in place at lower redshift, luminosity, and black-hole mass, confirming the universal nature of the X-ray emission mechanism in quasars. Even so, when compared against the well-known LX-LUV correlation, our quasars show an unexpectedly varied behaviour, splitting into two distinct subsets. About two-thirds of the sources are clustered around the relation with a minimal scatter of 0.1dex, while the remaining one-third appear to be X-ray underluminous by factors of >3-10. Such a large incidence (~=25%) of X-ray weakness has never been reported in radio-quiet, non-broad absorption line (BAL) quasar samples. Several factors could contribute to enhancing the X-ray weakness fraction among our z~=3 blue quasars, including variability, mild X-ray obscuration, contamination from weak-line quasars, and missed BALs. However, the X-ray weak objects also have, on average, flatter spectra, with no clear evidence of absorption. Indeed, column densities in excess of a few x1022cm–2 can be ruled out for most of the sample. We suggest that, at least in some of our X-ray weak quasars, the corona might experience a radiatively inefficient phase due to the presence of a powerful accretion-disc wind, which substantially reduces the accretion rate through the inner disc and therefore also the availability of seed photons for Compton up-scattering. The origin of the deviations from the LX-LUV relation will be further investigated in a series of future studies.

Abstract Copyright: © ESO 2019

Journal keyword(s): quasars: general - quasars: supermassive black holes - galaxies: active - X-rays: galaxies

Simbad objects: 33

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Number of rows : 33
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 SDSS J103027.09+052455.0 QSO 10 30 27.092 +05 24 55.02   26.15 25.44     ~ 303 0
14 2MASS J11110130-1505183 QSO 11 11 01.3020327600 -15 05 18.519922896           ~ 16 0
15 2MASS J11112059+2437408 QSO 11 11 20.5860582552 +24 37 40.886982912   18.34 17.97     ~ 25 0
16 QSO J1143+3452 QSO 11 43 08.8809241248 +34 52 22.233156204   17.43 17.15     ~ 49 0
17 [VV2000] J114851.4+231340 QSO 11 48 51.4730628120 +23 13 40.438137576   18.77 18.29     ~ 26 0
18 2MASS J11591153+3134272 QSO 11 59 11.5313895000 +31 34 27.240076992   18.40 18.11     ~ 36 0
19 QSO J1201+0116 QSO 12 01 44.3649782736 +01 16 11.740001304   18.09 17.74 17.4   ~ 66 2
20 [VV2006] J122017.0+454941 QSO 12 20 17.0720096088 +45 49 41.104511544   19.39 18.85     ~ 30 0
21 QSO J1225+4831 QSO 12 25 18.66000 +48 31 16.3020   18.69 18.30     ~ 41 0
22 Z 244-18 bCG 12 26 15.69 +48 29 38.3   15.3       ~ 364 0
23 2MASS J12463704+2625005 QSO 12 46 37.0609409328 +26 25 00.309738432   18.18 17.83     ~ 24 0
24 LBQS 1244+1129 QSO 12 46 40.3700829816 +11 13 02.901704808     18.4     ~ 64 0
25 QSO J1342+0928 QSO 13 42 08.100 +09 28 38.36           ~ 145 0
26 [VV2006] J140747.2+645420 QSO 14 07 47.2332082608 +64 54 19.916965836   17.73 17.41     ~ 43 0
27 [VV2006] J142543.3+540619 QSO 14 25 43.3298905704 +54 06 19.327380048   18.64 18.22     ~ 46 0
28 QSO B1425+606 QSO 14 26 56.1849081360 +60 25 50.813373324   16.82 16.54     ~ 148 0
29 QSO J1459+0024 QSO 14 59 07.1942637720 +00 24 01.272819600   19.43 18.87     ~ 46 0
30 SDSS J150731.48+241910.8 QSO 15 07 31.4873309664 +24 19 10.782769152   19.93 19.60     ~ 19 0
31 [VV2006] J153201.6+370002 QSO 15 32 01.5985744128 +37 00 02.333276064   18.12 17.80     ~ 35 0
32 QSO J1712+5755 QSO 17 12 27.7465195944 +57 55 06.895257456   17.75 17.53     ~ 45 0
33 LBQS 2230-0015 QSO 22 34 08.9971751592 +00 00 01.703853180   18.09 17.39 17.3   ~ 142 0

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