ORGANIZACIÓN DEL DISCURSO
18. UN GOBIERNO SERIO, EFICAZ Y HONRADO NO MILAGROSO.
•
’RASS-SDSS Galaxy CLuster Surevy. I. The Catalog and the correlation of X-ray and
optical properties.’, Popesso, P., B¨ohringer, H., Brinkmann, J., Voges, W.; York, D.
G, 2004, A&A, 423, 449
Abstract:’For a detailed comparison of the appearance of cluster of galaxies in X-rays
and in the optical, we have compiled a comprehensive database of X-ray and optical
properties of a sample of clusters based on the largest available X-ray and optical sur-
veys: the ROSAT All Sky Survey (RASS) and the Sloan Digital Sky Survey (SDSS).
The X-ray galaxy clusters of this RASS-SDSS catalog cover a wide range of masses,
from groups of 10
12.5M
to massive clusters of 10
15Min the redshift range 0.002-0.45.
The RASS-SDSS sample comprises all the X-ray selected objects already observed by
the Sloan Digital Sky Survey (114 clusters). For each system we have uniformly de-
termined the X-ray (luminosity in the ROSAT band, bolometric luminosity, center
coordinates) and optical properties (Schechter luminosity function parameters, lumi-
nosity, central galaxy density, core, total and half-light radii). For a subsample of 53
clusters we have also compiled the temperatures and the iron abundances from the lit-
erature. The total optical luminosity can be determined with a typical uncertainty of
20% independent of the choice of local or global background subtraction. We searched
for parameters which provide the best correlation between the X-ray luminosity and
the optical properties and found that the z band luminosity determined within a cluster
aperture of 0.5 Mpc h
−170
provides the best correlation, with a scatter of about 60-70%.
The scatter decreases to less than 40% if the correlation is limited to the bright X-ray
clusters. The resulting correlation of
L
Xand
L
opin the z and i bands shows a loga-
rithmic slope of 0.38, a value not consistent with the assumption of a constant
M/L.
Consistency is found, however, for an M/L increasing with luminosity as suggested by
other observations. We also investigated the correlation between
L
opand the X-ray
temperature, obtaining the same result.’
•
’RASS-SDSS Galaxy Clusters Survey. II. A unified picture of the Cluster Luminosity
Function.’,Popesso, P., B¨ohringer, H., Romaniello, M., Voges, W., 2005, A&A, 433,
415
Abstract:’We constructed the composite luminosity function (LF) of clusters of galaxies
in the five SDSS photometric bands u,g,r,i and z from the RASS-SDSS galaxy cluster
catalog. Background and foreground galaxies are subtracted using both a local and a
global background correction to take in account the presence of large scale structures
and variations from field to field, respectively. The composite LF clearly shows two
components: a bright-end LF with a classical slope of -1.25 in each photometric band,
and a faint-end LF steeper (−2.1
≤
α
≤ −1.6) in the dwarf galaxy region. The
observed upturn of the faint galaxies has a location ranging from -16 +5log(h) in the
g band to -18.5 +5log(h) in the z band. To study the universality of the cluster LF we
compare the individual cluster LFs with the composite luminosity function. We notice
that, in agreement with the composite LF, a single Schechter component is not a good
fit for the majority of the clusters. We fit a Schechter function to the bright-end of
the individual clusters LFs in the magnitude region brighter than the observed upturn
of the dwarf galaxies. We observe that the distributions of the derived parameters is
close to a Gaussian around the value of the composite bright-end LF parameters with
a dispersion compatible with the statistical errors. We conclude that the bright-end of
the galaxy clusters is universal. To study the behavior of the individual faint-end LF
we define the Dwarf to Giant galaxy Ratio (DGR) of the single clusters. We notice
that the distribution of DGR has a spread much larger than the statistical errors.
Our conclusion is that the cluster luminosity function is not universal since the cluster
faint-end, differently from the bright-end, varies from cluster to cluster.’
•
’RASS-SDSS Galaxy Cluster Survey. III. Scaling relations of galaxy clusters.’, Popesso,
P., B¨ohringer, H., Romaniello, M., Voges, W., 2005, A&A, 433, 431
Abstract:’We use the RASS-SDSS galaxy cluster sample to compare the quality of
optical and X-ray luminosities as predictors of other cluster properties such as their
masses, temperatures, and velocity dispersions. We use the SDSS spectroscopic data
to estimate the velocity dispersions and the virial masses of a subsample of 69 clusters
within
r500
and
r200. The ASCA temperature of the intra-cluster medium,
T
X, is
retrieved from the literature for a subsample of 49 clusters. For this subsample we
estimate the cluster masses also by using the mass-temperature relation. We show
that the optical luminosity,
L
op, correlates with the cluster mass much better than the
X-ray luminosity,
L
X.
L
opcan be used to estimate the cluster mass with an accuracy
of 40% while
L
Xcan predict the mass only with a 55% accuracy. We show that
correcting
L
Xfor the effect of a cool core at the center of a cluster, lowers the scatter
of theL
X−M
relation only by 3%. We find that the scatter observed in theL
op−L
Xrelation is determined by the scatter of the
L
X−M
relation. The mass-to-light ratio
in the SDSSiband clearly increases with the cluster mass with a slope 0.2±0.08. The
optical and X-ray luminosities correlate in excellent way with bothT
Xand
σ
Vwith an
orthogonal scatter of 20% in both relations. Moreover,
L
opand
L
Xcan predict with
the same accuracy both variables. We conclude that the cluster optical luminosity is
a key cluster parameter since it can give important information about fundamental
cluster properties such as the mass, the velocity dispersion, and the temperature of the
intra-cluster medium.’
•
’RASS-SDSS Galaxy Cluater survey. IV. An ubiquitous dwarf galaxy population in
clusters.’, Popesso, P., Biviano, A., B¨ohringer, H., Romaniello, M., 2006, A&A, 445,
29
Abstract:’We analyze the Luminosity Functions (LFs) of a subsample of 69 clusters
from the RASS-SDSS galaxy cluster catalog. When calculated within the cluster phys-
ical sizes, given byr200
orr500, all the cluster LFs appear to have the same shape, well
fitted by a composite of two Schechter functions with a marked upturn and a steepening
at the faint-end. Previously reported cluster-to-cluster variations of the LF faint-end
slope are due to the use of a metric cluster aperture for computing the LF of clusters
of different masses.
We determine the composite LF for early- and late-type galaxies, where the typing is
based on the galaxyu−r
colors. The late-type LF is well fitted by a single Schechter
function with a steep slope (α
=
−2.0 in the
r
band, within
r200). The early-type
LF instead cannot be fitted by a single Schechter function, and a composite of two
Schechter functions is needed. The faint-end upturn of the global cluster LF is due
to the early-type cluster galaxies. The shape of the bright-end tail of the early-type
LF does not seem to depend upon the local galaxy density or the distance from the
cluster center. The late-type LF shows a significant variation only very near the cluster
center. On the other hand, the faint-end tail of the early-type LF shows a significant
and continuous variation with the environment.
We provide evidence that the process responsible for creating the excess population
of dwarf early type galaxies in clusters is a threshold process that occurs when the
density exceeds
∼500 times the critical density of the Universe.
We interpret our results in the context of the ’harassment’ scenario, where faint early-
type cluster galaxies are predicted to be the descendants of tidally-stripped late-type
galaxies.’
•
,RASS-SDSS Galaxy Cluster survey. V. The Abell X-ray Underlumious Clusters.’, P.
Popesso, A. Biviano, H. B¨ohringer, M. Romaniello, 2007, A&A, 461, 397
Abstract:’In this paper we consider a large sample of optically selected clusters, in order
to elucidate the physical reasons for the existence of X-ray underluminous clusters.
For this purpose we analyzed the correlations of the X-ray and optical properties of
a sample of 137 spectroscopically confirmed Abell clusters in the SDSS database. We
searched for the X-ray counterpart of each cluster in the ROSAT All Sky Survey. We
find that 40% of our clusters have a marginal X-ray detection or remain undetected in
X-rays. These clusters appear too X-ray faint on average for their mass as determined
by velocity dispersion; i.e. they do not follow the scaling relation between X-ray
luminosity and virial mass traced by the other clusters. On the other hand, they do
follow the general scaling relation between optical luminosity and virial mass. We
refer to these clusters as the X-ray-underluminous Abell clusters (AXU clusters, for
short) and designate as ‘normal’ the X-ray detected Abell systems. We separately
examined the distributions and properties of the galaxy populations of the normal and
the AXU clusters. The AXU clusters are characterized by leptokurtic (more centrally
concentrated than a Gaussian) velocity distribution of their member galaxies in the
outskirts (1.5
< r/r200
≤
3.5), as expected for the systems in accretion. In addition,
the AXU clusters have a higher fraction of blue galaxies in the external region and show
a marginally significant paucity of galaxies at the center. Our results seem to support
the interpretation that the AXU clusters are systems in formation undergoing a phase
of mass accretion. Their low X-ray luminosity should be due to the still accreting
intracluster gas or to an ongoing merging process.’
•
’RASS-SDSS Galaxy Cluster survey. VI. The dependence of the cluster SFR on the
cluster global properties.’, P. Popesso, A. Biviano, M. Romaniello, H. B¨ohringer, 2007,
A&A, 461, 411
Abstract: ,To quantify the relationships between star formation in cluster galaxies and
global cluster properties. Using a subsample of 79 nearby clusters from the RASS-SDSS
galaxy cluster catalogue of Popesso et al. (2005a), we perform a regression analysis
between the cluster integrated star formation rate (ΣSF R) the cluster total stellar mass
(M
?), the fractions of star forming (f
SF) and blue (f
b) galaxies and other cluster global
properties, namely its richness (N
gal, i.e. the total number of cluster members within
the cluster virial radius, corrected for incompleteness), velocity dispersion (σ
v), virial
mass (M200), and X-ray luminosity (L
X). All cluster global quantities are corrected for
projection effects before the analysis. GalaxySF Rs and stellar masses are taken from
the catalog of Brinchmann et al. (2004), which is based on SDSS spectra. We only
consider galaxies with
M
r≤ −20.25 in our analysis, and exclude AGNs. We find that
both ΣSF R
and
M
?are correlated with all the cluster global quantities. A partial
correlation analysis show that all the correlations are induced by the fundamental one
between ΣSF R
and
N
gal, hence there is no evidence that the cluster properties affect
the mean
SF R
orM
?per galaxy. The relations between ΣSF R
and
M
?, on one side,
and both
N
galand
M200, on the other side, are linear, i.e. we see no evidence that
different clusters have different
SF R
or different
M
?per galaxy and per unit mass.
The fraction
f
SFdoes not depend on any cluster property considered, while
f
bdoes
depend on
L
X. We note that a significant fraction of star-forming cluster galaxies
are red (∼
25% of the whole cluster galaxy population). We conclude that the global
cluster properties are unable to affect the
SF
properties of cluster galaxies, but the
presence of the X-ray luminous intra-cluster medium can affect their colors, perhaps
through the ram-pressure stripping mechanism.’
•
’RASS-SDSS Galaxy Cluster survey. VII. On the Cluster Mass to Light ratio and
Halo Occupation Number.’ P. Popesso, A. Biviano, M. Romaniello, H. B¨ohringer,
2007, astro-ph/0606260, A&A in press
Abstract:’We explore the mass-to-light ratio in galaxy clusters and its relation to the
cluster mass. We study the relations among the optical luminosity (L
op), the cluster
mass (M200) and the number of cluster galaxies within
r200
(N
gal) in a sample of 217
galaxy clusters with confirmed 3D overdensity. We correct for projection effect, by
determining the galaxy surface number density profile in our cluster sample. This is
best fitted by a cored King profile in low and intermediate mass systems. The core
radius decreases with cluster mass, and, for the highest mass clusters, the profile is
better represented by a generalized King profile or a cuspy Navarro, Frenk & White
profile. We find a very tight proportionality betweenL
opandN
gal, which, in turn, links
the cluster mass-to-light ratio to the Halo Occupation DistributionN
galvs.
M200. After
correcting for projection effects, the slope of theL
op−M200
and
N
gal−M200
relations
is found to be 0.92±0.03, close, but still significantly less than unity. We show that
the non-linearity of these relations cannot be explained by variations of the galaxy
luminosity distributions and of the galaxy M/L with the cluster mass. We suggest
that the nonlinear relation between number of galaxies and cluster mass reflects an
underlying nonlinear relation between number of subhaloes and halo mass.
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Aproximación al análisis crítico del discurso político Un estudio de caso
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