790 research outputs found
A population of intermediate-mass black holes in dwarf starburst galaxies up to redshift=1.5
We study a sample of 50,000 dwarf starburst and late-type galaxies
drawn from the COSMOS survey with the aim of investigating the presence of
nuclear accreting black holes (BHs) as those seed BHs from which supermassive
BHs could grow in the early Universe. We divide the sample into five complete
redshift bins up to and perform an X-ray stacking analysis using the
\textit{Chandra} COSMOS-Legacy survey data. After removing the contribution
from X-ray binaries and hot gas to the stacked X-ray emission, we still find an
X-ray excess in the five redshift bins that can be explained by nuclear
accreting BHs. This X-ray excess is more significant for . At higher
redshifts, these active galactic nuclei could suffer mild obscuration, as
indicated by the analysis of their hardness ratios. The average nuclear X-ray
luminosities in the soft band are in the range 10 erg s.
Assuming that the sources accrete at 1\% the Eddington rate, their BH
masses would be 10 M, thus in the intermediate-mass BH
regime, but their mass would be smaller than the one predicted by the
BH-stellar mass relation. If instead the sources follow the correlation between
BH mass and stellar mass, they would have sub-Eddington accreting rates of
10 and BH masses 1-9 10 M. We thus
conclude that a population of intermediate-mass BHs exists in dwarf starburst
galaxies, at least up to =1.5, though their detection beyond the local
Universe is challenging due to their low luminosity and mild obscuration unless
deep surveys are employed.Comment: 10 pages, 7 figures, ApJ in pres
Heating of the IGM
Using the cosmic virial theorem, Press-Schechter analysis and numerical
simulations, we compute the expected X-ray background (XRB) from the diffuse
IGM with the clumping factor expected from gravitational shock heating. The
predicted fluxes and temperatures are excluded from the observed XRB. The
predicted clumping can be reduced by entropy injection. The required energy is
computed from the two-point correlation function, as well as from
Press-Schechter formalisms. The minimal energy injection of 1 keV/nucleon
excludes radiative or gravitational heating as a primary energy source. We
argue that the intergalactic medium (IGM) must have been heated through violent
processes such as massive supernova bursts. If the heating proceeded through
supernova explosions, it likely proceeded in bursts which may be observable in
high redshift supernova searches. Within our model we reproduce the observed
cluster luminosity-temperature relation with energy injection of 1 keV/nucleon
if this injection is assumed to be uncorrelated with the local density. These
parameters predict that the diffuse IGM soft XRB has a temperature of ~1 keV
with a flux near 10 keV/cm^2 s str keV, which may be detectable in the near
future.Comment: to appear in ApJ Lett., 11 pages incl 1 figur
The Multiphase Intracluster Medium in Galaxy Groups Probed by the Lyman Alpha Forest
The case is made that the intracluster medium (ICM) in spiral-rich galaxy
groups today probably has undergone much slower evolution than that in
elliptical-rich groups and clusters. The environments of proto-clusters and
proto-groups at z > 2 are likely similar to spiral-rich group environments at
lower redshift. Therefore, like the ICM in spiral-rich groups today, the ICM in
proto-groups and proto-clusters at z > 2 is predicted to be significantly
multiphased. The QSO Lyman alpha forest in the vicinity of galaxies is an
effective probe of the ICM at a wide range of redshift. Two recent observations
of Lyman alpha absorption around galaxies by Adelberger et al. and by
Pascarelle et al are reconciled, and it is shown that observations support the
multiphase ICM scenario. Galaxy redshifts must be very accurate for such
studies to succeed. This scenario can also explain the lower metallicity and
lower hot gas fraction in groups.Comment: 4 pages, 1 figure, replaced with the version after proo
The BeppoSAX view of the hard X-ray background
First results on a medium-deep X-ray survey in the "new" 5-10 keV band
carried out with the MECS detectors onboard BeppoSAX are presented. The High
Energy Llarge Area Survey (HELLAS) is aimed to directly explore a band where
the energy density of the X-ray background is more than twice than that in the
soft (0.5-2.0 keV) band. The optical identification follow-up of the first ten
HELLAS hard X-ray sources indicate that Active Galactic Nuclei are the dominant
population at 5-10 keV fluxes of the order of 10e-13 cgs. We discuss the
implications of these findings for the AGN synthesis models for the XRB.Comment: 6 pages, 4 figures, uses psfig.sty. Accepted for publication in
Advances in Space Research, Proceedings of the 32nd Scientific Assembly of
COSPA
Occupation of X-ray selected galaxy groups by X-ray AGN
We present the first direct measurement of the mean Halo Occupation
Distribution (HOD) of X-ray selected AGN in the COSMOS field at z < 1, based on
the association of 41 XMM and 17 C-COSMOS AGN with member galaxies of 189 X-ray
detected galaxy groups from XMM and Chandra data. We model the mean AGN
occupation in the halo mass range logM_200[Msun] = 13-14.5 with a rolling-off
power-law with the best fit index alpha = 0.06(-0.22;0.36) and normalization
parameter f_a = 0.05(0.04;0.06). We find the mean HOD of AGN among central
galaxies to be modelled by a softened step function at logMh > logMmin = 12.75
(12.10,12.95) Msun while for the satellite AGN HOD we find a preference for an
increasing AGN fraction with Mh suggesting that the average number of AGN in
satellite galaxies grows slower (alpha_s < 0.6) than the linear proportion
(alpha_s = 1) observed for the satellite HOD of samples of galaxies. We present
an estimate of the projected auto correlation function (ACF) of galaxy groups
over the range of r_p = 0.1-40 Mpc/h at = 0.5. We use the large-scale
clustering signal to verify the agreement between the group bias estimated by
using the observed galaxy groups ACF and the value derived from the group mass
estimates. We perform a measurement of the projected AGN-galaxy group
cross-correlation function, excluding from the analysis AGN that are within
galaxy groups and we model the 2-halo term of the clustering signal with the
mean AGN HOD based on our results.Comment: Accepted for publication in The Astrophysical Journa
The Chandra survey of the COSMOS field II: source detection and photometry
The Chandra COSMOS Survey (C-COSMOS) is a large, 1.8 Ms, Chandra program,
that covers the central contiguous ~0.92 deg^2 of the COSMOS field. C-COSMOS is
the result of a complex tiling, with every position being observed in up to six
overlapping pointings (four overlapping pointings in most of the central ~0.45
deg^2 area with the best exposure, and two overlapping pointings in most of the
surrounding area, covering an additional ~0.47 deg^2). Therefore, the full
exploitation of the C-COSMOS data requires a dedicated and accurate analysis
focused on three main issues: 1) maximizing the sensitivity when the PSF
changes strongly among different observations of the same source (from ~1
arcsec up to ~10 arcsec half power radius); 2) resolving close pairs; and 3)
obtaining the best source localization and count rate. We present here our
treatment of four key analysis items: source detection, localization,
photometry, and survey sensitivity. Our final procedure consists of a two step
procedure: (1) a wavelet detection algorithm, to find source candidates, (2) a
maximum likelihood Point Spread Function fitting algorithm to evaluate the
source count rates and the probability that each source candidate is a
fluctuation of the background. We discuss the main characteristics of this
procedure, that was the result of detailed comparisons between different
detection algorithms and photometry tools, calibrated with extensive and
dedicated simulations.Comment: Accepted for publication in The Astrophysical Journal Supplement
Serie
Probing Electron-Capture Supernovae: X-Ray Binaries in Starbursts
Presenting population models of high-mass X-ray binaries (HMXBs) formed after
bursts of star formation, we investigate the effect of electron-capture
supernovae (ECS) of massive ONeMg white dwarfs and the hypothesis that ECS
events are associated with typically low supernova kicks imparted to the
nascent neutron stars. We identify an interesting ECS bump in the time
evolution of HMXB numbers; this bump is caused by significantly increased
production of wind-fed HMXBs 20-60 Myr post starburst. The amplitude and age
extent of the ECS bump depend on the strength of ECS kicks and the mass range
of ECS progenitors. We also find that ECS-HMXBs form through a specific
evolutionary channel that is expected to lead to binaries with Be donors in
wide orbits. These characteristics, along with their sensitivity to ECS
properties, provide us with an intriguing opportunity to probe ECS physics and
progenitors through studies of starbursts of different ages. Specifically, the
case of the Small Magellanic Cloud, with a significant observed population of
Be HMXBs and starburst activity 30-60 Myr ago, arises as a promising laboratory
for understanding the role of electron-capture supernovae in neutron star
formation.Comment: 5 pages, 3 figures, Published by ApJ in 07/0
The Possible White Dwarf-Neutron Star Connection
The current status of the problem of whether neutron stars can form, in close
binary systems, by accretion-induced collapse (AIC) of white dwarfs is
examined. We find that, in principle, both initially cold C+O white dwarfs in
the high-mass tail of their mass distribution in binaries and O+Ne+Mg white
dwarfs can produce neutron stars. Which fractions of neutron stars in different
types of binaries (or descendants from binaries) might originate from this
process remains uncertain.Comment: 6 pages. To appear in "White Dwarfs", ed. J. Isern, M. Hernanz, and
E. Garcia-Berro (Dordrecht: Kluwer
The Population of High-Redshift Active Galactic Nuclei in the CHANDRA-Cosmos Survey
We present the high-redshift (3 3. Eighty-one sources are selected in the 0.5-2 keV band, fourteen are selected in the 2-10 keV and six in the 0.5-10 keV bands. We sample the high-luminosity (log L_((2-10keV)) > 44.15 erg s^(â1)) space density up to z ~ 5 and a fainter luminosity range (43.5 erg s^(â1) 3. We find that the space density of high-luminosity AGNs declines exponentially at all the redshifts, confirming the trend observed for optically selected quasars. At lower luminosity, the measured space density is not conclusive, and a larger sample of faint sources is needed. Comparisons with optical luminosity functions and black hole formation models are presented together with prospects for future surveys
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