2006AJ....131...55G


Query : 2006AJ....131...55G

2006AJ....131...55G - Astron. J., 131, 55-69 (2006/January-0)

XMM-Newton observations of high-redshift quasars.

GRUPE D., MATHUR S., WILKES B. and OSMER P.

Abstract (from CDS):

We report on our XMM-Newton observations of the high-redshift quasars BR 2237-0607 (z=4.558) and BR 0351-1034 (z=4.351). We also report on XMM-Newton observations of 19 other z>4 objects available in the public archive of which 14 were detected. We find that the optical to X-ray spectral index αox is correlated with the luminosity density at 2500 Å but does not show a correlation with redshift, which is consistent with earlier results. Radio-loud quasars are brighter and have flatter X-ray slopes compared to radio-quiet quasars. There is some evidence for the jet-dominated sources to be intrinsically absorbed. The mean intrinsic 2-10 keV power-law slope of the 10 high-redshift radio-quiet quasars in our sample for which a spectral analysis can be performed is αX=1.21±0.52 (ranging between 0.32 and 1.96), which is more like the αX=1.19±0.10 found from the ASCA observations of low-redshift narrow-line Seyfert 1 galaxies (NLS1s) but different from the αX=0.78±0.11 found for low-redshift broad-line Seyfert galaxies. The steep X-ray spectral index suggests high Eddington ratios L/LEdd. These observations give credence to the hypothesis of Mathur that NLS1s are low-luminosity cousins of high-redshift quasars. Comparison with other results from the literature indicates that perhaps the most luminous quasars, from low to high redshift, have similarly steep X-ray spectra suggestive of high Eddington luminosities.

Abstract Copyright:

Journal keyword(s): Galaxies: Active - Galaxies: Quasars: General - quasars: individual (BR 2237-0607) - Galaxies: Quasars: Individual: Alphanumeric: BR 0351-1034

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 QSO J0003-2603 QSO 00 03 22.9531962024 -26 03 18.304471908   18 17.53     ~ 291 0
2 QSO J0040-0915 BLL 00 40 54.6575670840 -09 15 26.833615164   26.46 22.40     ~ 58 0
3 QSO B0103+00 QSO 01 06 19.2392271120 +00 48 23.369353992   21.68 20.23     ~ 94 0
4 QSO J0248+1802 QSO 02 48 54.2720204400 +18 02 49.274967876     18.4     ~ 47 0
5 QSO B0351-1034 QSO 03 53 46.9729812432 -10 25 18.977437308     18.7     ~ 32 0
6 QSO J0525-3343 QSO 05 25 06.1749810960 -33 43 05.643939828     18.50 18.5   ~ 59 1
7 QSO B1026-084 QSO 10 28 38.79646593 -08 44 38.5362663     21.00 19.6   ~ 72 1
8 SDSS J103027.09+052455.0 QSO 10 30 27.092 +05 24 55.02   26.15 25.44     ~ 269 0
9 QSO B1033-033 QSO 10 36 23.7457432848 -03 43 18.929156772     18.5     ~ 73 0
10 SDSS J104433.04-012502.0 QSO 10 44 33.040 -01 25 02.08     21.81     ~ 175 1
11 [VV98] J105225.9+571907 QSO 10 52 25.88 +57 19 06.7   25.90 23.85 24.7 21.77 ~ 18 1
12 CXOHDFN J123642.1+621332 AGN 12 36 42.093 +62 13 31.29 26.61 27.03 26.43 25.8 25.7254 ~ 72 0
13 [VV2006] J123647.9+620940 QSO 12 36 47.95 +62 09 41.5 25.74 25.0 26.2 24.0 23.8871 ~ 37 0
14 CXOHDFN J123719.0+621025 SyG 12 37 18.98 +62 10 25.8   27.9 27.54 25.6 26.4494 ~ 19 0
15 [VV2006] J125304.0-090737 QSO 12 53 04.0 -09 07 37     23.65   22.98 ~ 6 0
16 QSO J1401+0244 QSO 14 01 46.5361320120 +02 44 34.755692604   22.03 20.32     ~ 51 0
17 7C 1428+4218 QSO 14 30 23.74163471 +42 04 36.4910561   24.43 22.04 20.2   ~ 145 1
18 QSO B1508+572 QSO 15 10 02.92237321 +57 02 43.3759220   22.73 21.38 19.23   ~ 202 0
19 QSO J1759+6638 QSO 17 59 28.0940839824 +66 38 52.633688352     21.9 20.220   ~ 31 0
20 [VV2006] J213945.0-234656 QSO 21 39 45.0 -23 46 56     22.87     ~ 7 0
21 QSO B2237-0607 QSO 22 39 53.6812264896 -05 52 19.996061772     18.3     ~ 118 0

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