arXiv subjects

I. Georgantopoulos

Publications and source records attributed to I. Georgantopoulos.

168 records · Page 10Linked to original sources

arXiv1997

Faint galaxies and the X-ray background

We summarise our recent work on the faint galaxy contribution to the cosmic X-ray background (XRB). At bright X-ray fluxes (in the ROSAT pass band), broad line QSOs dominate the X-ray source population, but at fainter fluxes there is evidence for a significant contribution from emission-line galaxies. Here we present statistical evidence that these galaxies can account for a large fraction of the XRB. We also demonstrate that these galaxies have significantly harder X-ray spectra than QSOs. Finally we present preliminary findings from infra-red spectroscopy on the nature of this X-ray emitting galaxy population. We conclude that a hybrid explanation consisting of obscured/Type 2 AGN surrounded by starburst activity can explain the properties of these galaxies and perhaps the origin of the entire XRB.

astro-ph↗

arXiv1997

A deep ROSAT Survey - XIV. X-ray emission from faint galaxies

We present a cross-correlation analysis to constrain the faint galaxy contribution to the cosmic X-ray background (XRB). Cross-correlating faint optical galaxy catalogues with unidentified X-ray sources from 3 deep ROSAT fields we find that B < 23 galaxies account for 20+-7 % of all X-ray sources to a flux limit of S(0.5-2.0 keV)=4x10^{-15} erg s-1 cm-2. To probe deeper, galaxies are then cross-correlated with the remaining unresolved X-ray images. A highly significant signal is obtained on each field. Allowing for the effect of the ROSAT point-spread function, and deconvolving the effect of galaxy clustering, we find that faint B < 23 galaxies directly account for 23+-3% of the unresolved XRB at 1keV. Using the optical magnitude of faint galaxies as probes of their redshift distribution, we find evidence for strong evolution in their X-ray luminosity, parameterised with the form L_x \propto (1+z)^3.2+-1.0. Extrapolation to z=2 will account for 40+-10% of the total XRB at 1keV. The nature of the emitting mechanism in these galaxies remains unclear, but we argue that obscured and/or low luminosity AGN provide the most natural explanation.

astro-ph↗

arXiv1997

ASCA observations of deep ROSAT fields I. the nature of the X-ray source populations

We present ASCA GIS observations (total exposure 100-200 ksec) of three fields which form part of our deep ROSAT survey. We detect 26 sources down to a limiting flux (2-10 keV) of 5x10^{-14} erg cm-2 s-1. Sources down to this flux level contribute 30 per cent of the 2-10 keV X-ray background. The number-count distribution, logN-logS, is a factor of three above the ROSAT counts, assuming a photon spectral index of 2 for the ROSAT sources. This suggests the presence at hard energies of a population other than the broad-line AGN which contribute to the ROSAT counts. This is supported by spectroscopic observations that show a large fraction of sources that are not obvious broad-line AGN. The average 1-10 keV spectral index of these sources is flat (0.92+-0.16), significantly different than that of the broad-line AGN (1.78+-0.16). Although some of the Narrow Emission Line Galaxies which are detected with ROSAT are also detected here, the nature of the flat spectrum sources remains as yet unclear.

astro-ph↗

arXiv1997

ROSAT observations of two 'cooling flow' EMSS Galaxies

We present ROSAT observations of two luminous L~10^44 erg/s EMSS galaxies, MS1019+5139 and MS1209+3917, previously classified as 'cooling flow' galaxies. MS1019+5139 does not appear to be spatially extended (<13 kpc) while its spectrum is well fit by a power law with Gamma = 1.73 +0.19-0.18; X-ray variability on a timescale of ~ years is also clearly detected. MS1209+3917 shows no evidence of spatial extension (<50 kpc) but it shows variability, while its spectrum can be fit with thermal bremsstrahlung emission (kT=1.8 +0.9-0.4 keV) or a power law model (Gamma = 2.50 +0.44-0.42, but with excess photoelectric absorption above the Galactic value). All the above argue against thermal emission from a group of galaxies or a galaxy but in favour of an AGN (possibly BL Lac) interpretation. We conclude that no 'normal' galaxies with high X-ray luminosities have yet been detected in the EMSS survey that could be significant contributors to the X-ray background.

astro-ph↗

arXiv1995

The discovery of a high redshift type 2 QSO

We report the discovery of a high redshift, narrow emission-line galaxy identified in the optical follow-up of deep ROSAT fields. The object has a redshift of z=2.35 and its narrow emission lines together with its high optical and X-ray luminosity imply that this is a rare example of a type 2 QSO. The intrinsic X-ray absorption is either very low or we are observing scattered flux which does not come directly from the nucleus. The X-ray spectrum of this object is harder than that of normal QSOs, and it is possible that a hitherto unidentified population of similar objects at fainter X-ray fluxes could account for the missing hard component of the X-ray background.

astro-ph↗

arXiv1994

A deep ROSAT survey - IV. The evolution of X-ray-selected QSOs

We report on a new estimate of the QSO X-ray luminosity function and its evolution with redshift based on a sample of 107 QSOs detected at faint X-ray fluxes, $S{\rm(0.5-2\,keV)}>4\times10^{-15}\,$\ergcms , with the {\it ROSAT} X-ray satellite. For $q_0=0.5$, the X-ray evolution of QSOs in this sample is consistent with strong luminosity evolution, $L_{\rm X} ^*(z) \propto (1+z)^{3.25\pm0.1}$, at low redshifts ($z<1.60$) and a constant comoving space density at higher redshifts. The derived rate of evolution at low redshifts is thus significantly higher than that obtained previously for the {\it Einstein} Extended Medium Sensitivity Survey (EMSS). Indeed, most luminosity evolution models provide a very poor fit (rejected at the 99 per cent confidence level) when applied to the combined EMSS and {\it ROSAT} samples, although a polynomial evolution model, $L_{\rm X} ^*(z) \propto 10^{(1.14\,z -0.23\,z^2)}$, provides an adequate fit for $q_0=0$. For $q_0=0.5$, a simple power-law luminosity evolution model with a redshift cut-off ($L_{\rm X} ^*(z) \propto (1+z)^{2.51\pm0.1}$,

astro-ph↗