2001MNRAS.327..499P


Query : 2001MNRAS.327..499P

2001MNRAS.327..499P - Mon. Not. R. Astron. Soc., 327, 499-506 (2001/October-3)

ASCA observations of deep ROSAT fields - V. The X-ray spectrum of hard X-ray selected QSOs.

PAPPA A., STEWART G.C., GEORGANTOPOULOS I., GRIFFITHS R.E., BOYLE B.J. and SHANKS T.

Abstract (from CDS):

We present an analysis of the ROSAT and ASCA spectra of 21 broad-line active galactic nuclei (AGN) quasi-stellar objects (QSOs) with z∼1 detected in the 2-10keV band with the ASCA GIS. The summed spectrum in the ASCA band is well described by a power law with Gamma=1.56±0.18, flatter than the average spectral index of bright QSOs and consistent with the spectrum of the X-ray background in this band. The flat spectrum in the ASCA band could be explained by only a moderate absorption (∼1022cm–2 assuming the typical AGN spectrum, i.e. a power law with Gamma=1.9. This could in principle suggest that some of the highly obscured AGN, required by most X-ray background synthesis models, may be associated with normal blue QSOs rather than narrow-line AGN. However, the combined 0.5-8keV ASCA-ROSAT spectrum is well fit by a power-law of Gamma=1.7±0.2 with a spectral upturn at soft energies. It has been pointed out that such an upturn may be an artefact of uncertainties in the calibration of the ROSAT or ASCA detectors. Nevertheless, if real, it could imply that the above absorption model suggested by the ASCA data alone is ruled out. Then a large fraction of QSOs could have `concave' spectra i.e. they gradually steepen towards softer energies. This result is in agreement with the BeppoSAX hardness ratio analysis of ∼100 hard X-ray selected sources.

Abstract Copyright: The Royal Astronomical Society

Journal keyword(s): surveys - galaxies: active - quasars: general - X-rays: general

Simbad objects: 22

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Number of rows : 22
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 AX J0050.8-2902 QSO 00 50 53.8 -29 02 16           ~ 1 0
2 AX J0051.9-2913 QSO 00 51 56.7 -29 13 56           ~ 1 0
3 AX J0053.0-2927 QSO 00 53 05.1 -29 11 39           ~ 1 0
4 QSO B0053.9-2805 QSO 00 56 23.6379170976 -27 48 56.018697264   17.86       ~ 9 0
5 [VV2006] J005634.0-272951 QSO 00 56 34.0328 -27 29 50.666   16.9   17.375   ~ 8 0
6 QSO B0054-2748 QSO 00 57 24.5027046048 -27 32 00.808346040   19.5       ~ 17 0
7 RX J0057.7-2735 QSO 00 57 48.5 -27 35 56           ~ 3 0
8 QSO B0339-4422 QSO 03 41 04.2733714056 -44 12 05.253661044     21.6     ~ 8 0
9 [VV2006c] J034119.3-441030 Sy1 03 41 16 -44 10.2   21.5 21.55     ~ 8 0
10 QSO B0340-4413 QSO 03 42 03.7361116008 -44 03 45.196670844   19.2       ~ 13 0
11 QSO B0340-4419 QSO 03 42 05.5590514392 -44 09 42.371678844     21.3     ~ 8 0
12 [VV98] J034219.4-440238 QSO 03 42 20.1 -44 12 30   21.8 21.8     ~ 8 3
13 [VV96] J034226.2-451305 QSO 03 42 25.8496030776 -45 13 11.533550916   18.27 18.27     ~ 8 0
14 AX J0342.5-4502 QSO 03 42 35.0 -45 02 19           ~ 1 0
15 1AXG J034233-4403 QSO 03 42 38.5609551384 -44 04 49.162456128   20.4       ~ 12 0
16 Shanks QSF1X:071 QSO 03 43 18.0 -44 51 37   22.16       ~ 5 0
17 [VV98] J104605.1-002048 QSO 10 46 05.8832424024 -00 20 25.324293696   20.24 19.85     ~ 10 0
18 QSO B1043-0006 QSO 10 46 14.9437778256 -00 22 48.482737320   20.40 20.14     ~ 14 0
19 [VV96] J134325.8-001613 QSO 13 43 25.8412398744 -00 16 12.232787628   19.43 19.17     ~ 34 0
20 AX J1343.3-0016 QSO 13 43 51.8 -00 04 41           ~ 1 0
21 3XMM J134459.4-001559 Sy1 13 44 59.4488776152 -00 15 59.514719292   17.83 17.64     ~ 57 0
22 NGC 5548 Sy1 14 17 59.5400291832 +25 08 12.603122268   14.35 13.73     ~ 2895 0

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