2019A&A...630A.118V


Query : 2019A&A...630A.118V

2019A&A...630A.118V - Astronomy and Astrophysics, volume 630A118-118 (2019/10-1)

The X-ray properties of z > 6 quasars: no evident evolution of accretion physics in the first Gyr of the Universe.

VITO F., BRANDT W.N., BAUER F.E., CALURA F., GILLI R., LUO B., SHEMMER O., VIGNALI C., ZAMORANI G., BRUSA M., CIVANO F., COMASTRI A. and NANNI R.

Abstract (from CDS):


Context. X-ray emission from quasars (QSOs) has been used to assess supermassive black hole accretion properties up to z~=6. However, at z>6 only ~=15 QSOs are covered by sensitive X-ray observations, preventing a statistically significant investigation of the X-ray properties of the QSO population in the first Gyr of the Universe.
Aims. We present new Chandra observations of a sample of 10 z>6 QSOs, selected to have virial black-hole mass estimates from MgII line spectroscopy (logMBH/M☉=8.5-9.6). Adding archival X-ray data for an additional 15 z>6 QSOs, we investigate the X-ray properties of the QSO population in the first Gyr of the Universe. In particular, we focus on the LUV-LX relation, which is traced by the αox parameter, and the shape of their X-ray spectra.
Methods. We performed photometric analyses to derive estimates of the X-ray luminosities of our z>6 QSOs, and thus their αox values and bolometric corrections (Kbol=Lbol/LX). We compared the resulting αox and Kbol distributions with the results found for QSO samples at lower redshift, and ran several statistical tests to check for a possible evolution of the LUV-LX relation. Finally, we performed a basic X-ray spectral analysis of the brightest z>6 QSOs to derive their individual photon indices, and joint spectral analysis of the whole sample to estimate the average photon index.
Results. We detect seven of the new Chandra targets in at least one standard energy band, while two more are detected discarding energies E>5keV, where background dominates. We confirm a lack of significant evolution of αox with redshift, which extends the results from previous works up to z>6 with a statistically significant QSO sample. Furthermore, we confirm the trend of an increasing bolometric correction with increasing luminosity found for QSOs at lower redshifts. The average power-law photon index of our sample (<Γ> =2.20–0.34+0.39 and <Γ≥2.13–0.13+0.13 for sources with <30 and >30 net counts, respectively) is slightly steeper than, but still consistent with, typical QSOs at z=1-6.
Conclusions. All of these results indicate a lack of substantial evolution of the inner accretion-disk and hot-corona structure in QSOs from low redshift to z>6. Our data hint at generally high Eddington ratios at z>6.

Abstract Copyright: © ESO 2019

Journal keyword(s): methods: data analysis - galaxies: active - galaxies: nuclei - X-rays: galaxies - galaxies: high-redshift - quasars: general

Simbad objects: 28

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Number of rows : 28
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 [VV2006] J002822.8-283041 QSO 00 28 22.7737488480 -28 30 40.284581976     20.30     ~ 6 0
2 CFHQS J005006+344522 QSO 00 50 06.694 +34 45 21.79           ~ 47 0
3 SDSS J010013.02+280225.8 QSO 01 00 13.0246669824 +28 02 25.791716364           ~ 206 0
4 QSO J0109-3047 QSO 01 09 53.136 -30 47 26.30           ~ 56 0
5 QSO J0142-3327 QSO 01 42 43.720 -33 27 45.61           ~ 49 0
6 CFHQS J021013-045620 QSO 02 10 13.190 -04 56 20.79           ~ 61 0
7 CFHQS J021627-045534 QSO 02 16 27.81000 -04 55 34.0997           ~ 27 0
8 QSO J0226+0302 QSO 02 26 01.873 +03 02 59.24           ~ 89 0
9 SDSS J030331.40-001912.9 QSO 03 03 31.408 -00 19 12.99           ~ 44 0
10 QSO J0305-3150 QSO 03 05 16.918 -31 50 55.85           ~ 102 0
11 SDSS J084229.43+121850.4 QSO 08 42 29.438 +12 18 50.47           ~ 88 0
12 SDSS J103027.09+052455.0 QSO 10 30 27.092 +05 24 55.02   26.15 25.44     ~ 303 0
13 SDSS J104845.05+463718.3 QSO 10 48 45.058 +46 37 18.38   25.87 24.76     ~ 133 0
14 PSO J167.6415-13.4960 QSO 11 10 33.963 -13 29 45.73           ~ 45 0
15 QSO J1120+0641 QSO 11 20 01.463 +06 41 23.79           ~ 262 0
16 SDSS J114816.64+525150.3 QSO 11 48 16.647 +52 51 50.31   25.73 25.04     ~ 487 0
17 SDSS J130608.25+035626.3 QSO 13 06 08.259 +03 56 26.19   25.59 24.81     ~ 176 0
18 QSO J1342+0928 QSO 13 42 08.100 +09 28 38.36           ~ 145 0
19 CFHQS J150941-174926 QSO 15 09 41.77920 -17 49 26.7996           ~ 82 0
20 ULAS J153910.16+055749.7 QSO 15 39 10.16040 +05 57 49.7160           ~ 12 0
21 SDSS J160253.98+422824.8 QSO 16 02 53.982 +42 28 24.86   24.32 24.32     ~ 75 0
22 SDSS J162331.81+311200.5 QSO 16 23 31.806 +31 12 00.55   24.77 25.16     ~ 85 0
23 SDSS J163033.89+401209.6 QSO 16 30 33.898 +40 12 09.68   26.45 25.01     ~ 89 0
24 CFHQS J164121+375520 QSO 16 41 21.72833 +37 55 20.1464           ~ 37 0
25 QSO J2216-0016 QSO 22 16 44.47 -00 16 50.1           ~ 29 0
26 QSO J2232+2930 QSO 22 32 55.14497 +29 30 32.3136           ~ 42 0
27 SDSS J231038.88+185519.7 QSO 23 10 38.888 +18 55 19.72           ~ 107 0
28 ULAS J231556.23+014350.3 QSO 23 15 56.236 +01 43 50.38           ~ 18 0

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