2023A&A...678A.201Z


Query : 2023A&A...678A.201Z

2023A&A...678A.201Z - Astronomy and Astrophysics, volume 678A201 (2023/10-1)

HYPerluminous quasars at the Epoch of ReionizatION (HYPERION): A new regime for the X-ray nuclear properties of the first quasars.

ZAPPACOSTA L., PICONCELLI E., FIORE F., SACCHEO I., VALIANTE R., VIGNALI C., VITO F., VOLONTERI M., BISCHETTI M., COMASTRI A., DONE C., ELVIS M., GIALLONGO E., LA FRANCA F., LANZUISI G., LAURENTI M., MINIUTTI G., BONGIORNO A., BRUSA M., CIVANO F., CARNIANI S., D'ODORICO V., FERUGLIO C., GALLERANI S., GILLI R., GRAZIAN A., GUAINAZZI M., MARINUCCI A., MENCI N., MIDDEI R., NICASTRO F., PUCCETTI S., TOMBESI F., TORTOSA A., TESTA V., VIETRI G., CRISTIANI S., HAARDT F., MAIOLINO R., SCHNEIDER R., TRIPODI R., VALLINI L. and VANZELLA E.

Abstract (from CDS):

The existence of luminous quasars (QSOs) at the epoch of reionization (EoR; i.e., z > 6) powered by well-grown supermassive black holes (SMBHs) with masses ≳109 M⊙ challenges models of early SMBH formation and growth. To shed light on the nature of these sources, we started a multiwavelength program based on a sample of 18 HYPerluminous quasars at the Epoch of ReionizatION (HYPERION). These are the luminous QSOs whose SMBHs must have had the most rapid mass growth during the first gigayear of the Universe and therefore acquired the largest mass at their respective epochs. In this paper, we present the HYPERION sample and report results from the first year of the planned three years of observations of the 2.4 Ms XMM-Newton Multi-Year Heritage program on which HYPERION is based. The goal of this program is to accurately characterise the X-ray nuclear properties of QSOs at the EoR. Through a joint X-ray spectral analysis of ten sources, covering the rest-frame ∼2 - 50 keV energy range, we report a steep average photon index (Γ ≈ 2.4 ± 0.1). No absorption is required at levels of 1021 - 1022 cm–2. The measured average Γ is inconsistent at ≥4σ level with the canonical value (Γ = 1.8 - 2) measured in QSOs at z < 6. Such a steep spectral slope is also significantly steeper than that reported in lower-z analog QSOs with similar luminosity or accretion rate, suggesting genuine redshift evolution. Alternatively, we can interpret this result as suggesting the presence of a very low energy cutoff Ecut ≈ 20 keV on a standard Γ = 1.9 power-law, the likes of which is rarely reported at lower z. We also report mild indications that, on average, HYPERION QSOs show higher levels of coronal soft X-rays at 2 keV compared to the accretion disk UV at 2500 Å than expected for lower-z AGN in the high-luminosity regime. We speculate that either a redshift-dependent coupling between the X-ray corona and accretion disk or intrinsically different coronal properties account for the steepness of the X-ray spectral slope, especially in the presence of powerful winds. The reported steep slopes, if confirmed in lower-luminosity regimes, may have an important impact on the design of next-generation X-ray facilities and future surveys designed to investigate the early Universe.

Abstract Copyright: © The Authors 2023

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

Simbad objects: 20

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Number of rows : 20
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 J0020-3653 QSO 00 20 31.46969 -36 53 41.8114           ~ 25 0
2 QSO J0038-1527 QSO 00 38 36.09984 -15 27 23.5998           ~ 30 0
3 QSO J0045+0901 QSO 00 45 33.56800 +09 01 56.9600           ~ 21 0
4 CFHQS J005006+344522 QSO 00 50 06.694 +34 45 21.79           ~ 47 0
5 SDSS J010013.02+280225.8 QSO 01 00 13.0246669824 +28 02 25.791716364           ~ 206 0
6 QSO J0142-3327 QSO 01 42 43.720 -33 27 45.61           ~ 49 0
7 VST-ATLAS J015957.96-363356.8 QSO 01 59 57.97150 -36 33 56.6028           ~ 29 0
8 VDES J0224-4711 QSO 02 24 26.54 -47 11 29.4           ~ 50 0
9 QSO J0226+0302 QSO 02 26 01.873 +03 02 59.24           ~ 89 0
10 QSO J0244-5008 QSO 02 44 01.02 -50 08 53.7           ~ 19 0
11 QSO J0252-0503 QSO 02 52 16.63999 -05 03 31.7999           ~ 31 0
12 VHS J0411-0907 QSO 04 11 28.62984 -09 07 49.8000           ~ 28 0
13 PSO J083.8371+11.8482 QSO 05 35 20.9 +11 50 54           ~ 9 0
14 QSO J1007+2115 QSO 10 07 58.26 +21 15 29.2           ~ 39 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 QSO J1342+0928 QSO 13 42 08.100 +09 28 38.36           ~ 145 0
18 CFHQS J142952+544717 QSO 14 29 52.16880 +54 47 17.6964           ~ 68 0
19 QSO J1526-2050 QSO 15 26 37.844 -20 50 00.88           ~ 78 0
20 RX J1927.3+6533 Sy2 19 27 19.5393064368 +65 33 54.335877408     15.4     ~ 147 0

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