7,331 research outputs found

    Evolution in the iron abundance of the ICM

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    We present a Chandra analysis of the X-ray spectra of 56 clusters of galaxies at z>0.3z>0.3, which cover a temperature range of 3>kT>153> kT > 15 keV. Our analysis is aimed at measuring the iron abundance in the ICM out to the highest redshift probed to date. We find that the emission-weighted iron abundance measured within (0.150.3)Rvir(0.15-0.3) R_{vir} in clusters below 5 keV is, on average, a factor of 2\sim2 higher than in hotter clusters, following Z(T)0.88T0.47ZZ(T)\simeq 0.88 T^{-0.47} Z_\odot, which confirms the trend seen in local samples. We made use of combined spectral analysis performed over five redshift bins at 0.3>z>1.30.3> z > 1.3 to estimate the average emission weighted iron abundance. We find a constant average iron abundance ZFe0.25ZZ_{Fe}\simeq 0.25 Z_\odot as a function of redshift, but only for clusters at z>0.5z>0.5. The emission-weighted iron abundance is significantly higher (ZFe0.4ZZ_{Fe}\simeq0.4 Z_\odot) in the redshift range z0.30.5z\simeq0.3-0.5, approaching the value measured locally in the inner 0.15Rvir0.15 R_{vir} radii for a mix of cool-core and non cool-core clusters in the redshift range 0.1<z<0.30.1<z<0.3. The decrease in ZFeZ_{Fe} with zz can be parametrized by a power law of the form (1+z)1.25\sim(1+z)^{-1.25}. The observed evolution implies that the average iron content of the ICM at the present epoch is a factor of 2\sim2 larger than at z1.2z\simeq 1.2. We confirm that the ICM is already significantly enriched (ZFe0.25ZZ_{Fe}\simeq0.25 Z_\odot) at a look-back time of 9 Gyr. Our data provide significant constraints on the time scales and physical processes that drive the chemical enrichment of the ICM.Comment: 4 pages, 4 figures, to appear in the Proceedings of "The Extreme Universe in the Suzaku Era", Dicember 2006, Kyoto (Japan

    A FIRST DETERMINATION OF THE SURFACE DENSITY OF GALAXY CLUSTERS AT VERY LOW X--RAY FLUXES

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    We present the first results of a serendipitous search for clusters of galaxies in deep ROSAT-PSPC pointed observations at high galactic latitude. The survey is being carried out using a Wavelet based Detection Algorithm which is not biased against extended, low surface brightness sources. A new flux--diameter limited sample of 10 cluster candidates has been created from 3deg2\rm\sim 3 \, deg^2 surveyed area. Preliminary CCD observations have revealed that a large fraction of these candidates correspond to a visible enhancement in the galaxy surface density, and several others have been identified from other surveys. We believe these sources to be either low--moderate redshift groups or intermediate to high redshift clusters. We show X-ray and optical images of some of the clusters identified to date. We present, for the first time, the derived number density of the galaxy clusters to a flux limit of 11014ergcm2s1\rm 1\cdot 10^{-14} erg cm^{-2} s^{-1} (0.5--2.0 keV). This extends the logN\log N--logS\log S of previous cluster surveys by more than one decade in flux. Results are compared to theoretical predictions for cluster number counts.Comment: uuencoded compressed Postscript, 7 pages including 4 figures. Accepted for publication in Ap. J. Letters

    The micro-Jy Radio Source Population: the VLA-CDFS View

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    We analyse the 267 radio sources from our deep (flux limit of 42 microJy at the field center at 1.4 GHz) Chandra Deep Field South 1.4 and 5 GHz VLA survey. The radio population is studied by using a wealth of multi-wavelength information, including morphology and spectral types, in the radio, optical, and X-ray bands. The availability of redshifts for ~ 70% of our sources allows us to derive reliable luminosity estimates for the majority of the objects. Contrary to some previous results, we find that star-forming galaxies make up only a minority (~ 1/3) of sub-mJy sources, the bulk of which are faint radio galaxies, mostly of the Fanaroff-Riley I type.Comment: 6 pages, 3 figures, to appear in the proceedings of "At the Edge of the Universe", Sintra, Portugal, Oct. 9 - 13, 200
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