2021A&A...653A.158L


Query : 2021A&A...653A.158L

2021A&A...653A.158L - Astronomy and Astrophysics, volume 653A158-158 (2021/9-1)

The most luminous blue quasars at 3.0 < z < 3.3. II. C IV/X-ray emission and accretion disc physics.

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

Abstract (from CDS):

We analyse the properties of the high-ionisation CIVλ1549 broad emission line in connection with the X-ray emission of 30 bright, optically selected quasars at z≃3.0-3.3 with pointed XMM-Newton observations, which were selected to test the suitability of active galactic nuclei as cosmological tools. In our previous work, we found that a large fraction (≃25%) of the quasars in this sample are X-ray under-luminous by factors of >3-10. As absorbing columns of ≥1023cm–2 can be safely ruled out, their weakness is most likely intrinsic. Here we explore possible correlations between the UV and X-ray features of these sources to investigate the origin of X-ray weakness with respect to X-ray-normal quasars at similar redshifts. We fit the UV spectra from the Sloan Digital Sky Survey of the quasars in our sample and analyse their CIV properties - for example equivalent width (EW) and line peak velocity (υpeak) - as a function of the X-ray photon index and 2-10keV flux. We confirm the statistically significant trends of CIVυpeak and EW with UV luminosity at 2500Å for both X-ray-weak and X-ray-normal quasars, as well as the correlation between X-ray weakness (parametrised through Δαox) and CIV EW. In contrast to some recent work, we do not observe any clear relation between the 2-10keV luminosity and υpeak. We find a statistically significant correlation between the hard X-ray flux and the integrated CIV flux for X-ray-normal quasars, which extends across more than three (two) decades in CIV (X-ray) luminosity, whilst X-ray-weak quasars deviate from the main trend by more than 0.5dex. We argue that X-ray weakness might be interpreted in a starved X-ray corona picture associated with an ongoing disc-wind phase. If the wind is ejected in the vicinity of the black hole, the extreme-UV radiation that reaches the corona will be depleted, depriving the corona of seed photons and generating an X-ray-weak quasar. Nonetheless, at the largest UV luminosities (>1047erg/s) there will still be an ample reservoir of ionising photons that can explain the 'excess' CIV emission observed in the X-ray-weak quasars with respect to normal sources of similar X-ray luminosities.

Abstract Copyright: © ESO 2021

Journal keyword(s): galaxies: active - quasars: general - quasars: supermassive black holes - methods: statistical

Simbad objects: 34

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Number of rows : 34
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 2MASS J09584122+2827291 QSO 09 58 41.2178328792 +28 27 29.568196188   19.02 18.44     ~ 24 0
12 QSO B1011+4315 QSO 10 14 47.1891688176 +43 00 30.167514324   17.39 17.05     ~ 74 0
13 [VV2000] J102714.7+354318 QSO 10 27 14.7800880984 +35 43 17.395124844   16.96 16.69     ~ 50 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 2MASS J12463704+2625005 QSO 12 46 37.0609409328 +26 25 00.309738432   18.18 17.83     ~ 24 0
23 LBQS 1244+1129 QSO 12 46 40.3700829816 +11 13 02.901704808     18.4     ~ 64 0
24 [VV2006] J140747.2+645420 QSO 14 07 47.2332082608 +64 54 19.916965836   17.73 17.41     ~ 43 0
25 [VV2006] J142124.0+463318 QSO 14 21 23.9850678432 +46 33 17.955577764   18.53 17.99     ~ 47 0
26 [VV2006] J142543.3+540619 QSO 14 25 43.3298905704 +54 06 19.327380048   18.64 18.22     ~ 46 0
27 QSO B1425+606 QSO 14 26 56.1849081360 +60 25 50.813373324   16.82 16.54     ~ 148 0
28 QSO J1459+0024 QSO 14 59 07.1942637720 +00 24 01.272819600   19.43 18.87     ~ 46 0
29 SDSS J150731.48+241910.8 QSO 15 07 31.4873309664 +24 19 10.782769152   19.93 19.60     ~ 19 0
30 QSO J1521+5202 QSO 15 21 56.4821480376 +52 02 38.598049752   16.02 15.70     ~ 64 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 PHL 1811 Sy1 21 55 01.5124437432 -09 22 24.349496808   13.9 16.8 14.1   ~ 200 1
34 LBQS 2230-0015 QSO 22 34 08.9971751592 +00 00 01.703853180   18.09 17.39 17.3   ~ 142 0

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