131 research outputs found
Globular Clusters in Dense Clusters of Galaxies
Deep imaging data from the Keck II telescope are employed to study the
globular cluster (GC) populations in the cores of six rich Abell clusters. The
sample includes A754, A1644, A2124, A2147, A2151, and A2152, and spans the
redshift range z = 0.035-0.066. The clusters also range in morphology from
spiral-rich, irregular systems to centrally concentrated cD clusters rich in
early-type galaxies. Globular cluster specific frequencies S_N and luminosity
function dispersions are measured for a total of 9 galaxies in six central
fields. The measured values of S_N for the six brightest cluster galaxies
(BCGs) are all higher than typical values for giant ellipticals, in accord with
the known S_N-density correlations. The three non-BCGs analyzed also have
elevated values of S_N, confirming that central location is a primary factor.
The number of GCs per unit mass for these fields are consistent with those
found in an earlier sample, giving further evidence that GC number scales with
mass and that the S_N variations are due to a deficit of halo light, i.e., S_N
reflects mass-to-light ratio.
The discussion builds on an earlier suggestion that the GCs (both metal rich
and metal poor) around the central cluster galaxies were assembled at early
times, and that star formation halted prematurely in the central galaxies at
the epoch of cluster collapse. This is consistent with recent simulations of
BCG/cluster formation. The subsequent addition of luminous material through
cluster dynamical evolution can cause S_N to decrease, and we may be seeing the
first evidence of this. Finally, the GC luminosity function measurements are
used to constrain the relative distances of the three clusters that make up the
Hercules supercluster.Comment: Uses emulateapj.sty (included); 17 pages with 9 included PostScript
figures. Figures 1-6 are separate GIF images (so 15 figures total) available
from http://astro.caltech.edu/~jpb/clusters -- the full PostScript version of
the paper (20 pages; 2.2 Mb compressed) incorporating Figures 1-6 can also be
grabbed from this URL. Accepted for publication in A
The Properties of Poor Groups of Galaxies: III. The Galaxy Luminosity Function
We obtain R-band photometry for galaxies in six nearby poor groups for which
we have spectroscopic data, including 328 new galaxy velocities. For the five
groups with luminous X-ray halos, the composite group galaxy luminosity
function (GLF) is fit adequately by a Schechter function with Mstar = -21.6 +/-
0.4 + 5log h and alpha = -1.3 +/- 0.1. We also find that (1) the ratio of
dwarfs to giants is significantly larger for the five groups with luminous
X-ray halos than for the one marginally X-ray detected group, (2) the composite
GLF for the luminous X-ray groups is consistent in shape with that for rich
clusters, (3) the composite group GLF rises more steeply at the faint end than
that of the field, (4) the shape difference between the field and composite
group GLF's results mostly from the population of non-emission line galaxies,
whose dwarf-to-giant ratio is larger in the denser group environment than in
the field, and (5) the non-emission line dwarfs are more concentrated about the
group center than the non-emission line giants. This last result indicates that
the dwarfs and giants occupy different orbits (i.e., have not mixed completely)
and suggests that the populations formed at a different times. Our results show
that the shape of the GLF varies with environment and that this variation is
due primarily to an increase in the dwarf-to-giant ratio of quiescent galaxies
in higher density regions, at least up to the densities characteristic of X-ray
luminous poor groups. This behavior suggests that, in some environments, dwarfs
are more biased than giants with respect to dark matter. This trend conflicts
with the prediction of standard biased galaxy formation models. (Abridged)Comment: 36 pages, AASLaTeX with 8 figures. Table 1 also available at
http://atropos.as.arizona.edu/aiz/papers/all_grp_lf_ascii.dat.final . To
appear in Ap
Deep near-infrared luminosity function of a cluster of galaxies at z=0.3
The deep near-infrared luminosity function of AC118, a cluster of galaxies at
z=0.3, is presented. AC118 is a bimodal cluster, as evidenced both by our
near-infrared images of lensed galaxies, by public X-ray Rosat images and by
the spatial distribution of bright galaxies. Taking advantage of the extension
and depth of our data, which sample an almost unexplored region in the depth
vs. observed area diagram, we derive the luminosity function (LF), down to the
dwarf regime (M*+5), computed in several cluster portions. The overall LF,
computed on a 2.66 Mpc2 areas (H_0=50 km/s/Mpc), has an intermediate slope
(alpha=-1.2). However, the LF parameters depend on the surveyed cluster region:
the central concentration has 2.6^{+5.1}_{-1.7} times more bright galaxies and
5.3^{+7.2}_{-2.3} times less dwarfs per typical galaxy than the outer region,
which includes galaxies at an average projected distance of ~580 kpc (errors
are quoted at the 99.9 % confidence level). The LF in the secondary AC118 clump
is intermediate between the central and outer one. In other words, the
near-infrared AC118 LF steepens going from high to low density regions. At an
average clustercentric distance of ~580 kpc, the AC118 LF is statistically
indistinguishable from the LF of field galaxies at similar redshift, thus
suggesting that the hostile cluster environment plays a minor role in shaping
the LF at large clustercentric distances, while it strongly affects the LF at
higher galaxy density.Comment: ApJ, in press. The whole paper with all high resolution images is
available at http://www.na.astro.it/~andreon/listapub.htm
Surface photometry of new nearby dwarf galaxies
We present CCD surface photometry of 16 nearby dwarf galaxies, many of which
were only recently discovered. Our sample comprises both isolated galaxies and
galaxies that are members of nearby galaxy groups. The observations were
obtained in the Johnson B and V bands (and in some cases in Kron-Cousins I). We
derive surface brightness profiles, total magnitudes, and integrated colors.
For the 11 galaxies in our sample with distance estimates the absolute B
magnitudes lie in the range of -10>Mb>-13. The central surface brightness
ranges from 22.5 to 27.0 mag/sq.arcsec. Most of the dwarf galaxies show
exponential light profiles with or without a central light depression.
Integrated radial color gradients, where present, appear to indicate a more
centrally concentrated younger population and a more extended older population.Comment: accepted by A&
Iron and s-elements abundance variations in NGC5286: comparison with anomalous globular clusters and Milky Way satellites
We present a high resolution spectroscopic analysis of 62 red giants in the
Milky Way globular cluster NGC5286. We have determined abundances of
representative light proton-capture, alpha, Fe-peak and neutron-capture element
groups, and combined them with photometry of multiple sequences observed along
the colour-magnitude diagram. Our principal results are: (i) a broad, bimodal
distribution in s-process element abundance ratios, with two main groups, the
s-poor and s-rich groups; (ii) substantial star-to-star Fe variations, with the
s-rich stars having higher Fe, e.g. _s-rich - _s-poor ~
0.2~dex; and (iii) the presence of O-Na-Al (anti-)correlations in both stellar
groups. We have defined a new photometric index, c_{BVI}=(B-V)-(V-I), to
maximise the separation in the colour-magnitude diagram between the two stellar
groups with different Fe and s-element content, and this index is not
significantly affected by variations in light elements (such as the O-Na
anticorrelation). The variations in the overall metallicity present in NGC5286
add this object to the class of "anomalous" GCs. Furthermore, the chemical
abundance pattern of NGC5286 resembles that observed in some of the anomalous
GCs, e.g. M22, NGC1851, M2, and the more extreme Omega Centauri, that also show
internal variations in s-elements, and in light elements within stars with
different Fe and s-elements content. In view of the common variations in
s-elements, we propose the term s-Fe-anomalous GCs to describe this sub-class
of objects. The similarities in chemical abundance ratios between these objects
strongly suggest similar formation and evolution histories, possibly associated
with an origin in tidally disrupted dwarf satellites.Comment: 28 pages, 21 figures, accepted for publication in MNRA
Accretion and nuclear activity of quiescent supermassive black holes. I: X-ray study
We have studied the nuclear activity in a sample of six quiescent early-type
galaxies, with new Chandra data and archival HST optical images. Their nuclear
sources have X-ray luminosities ~ 10^{38} - 10^{39} erg/s (L_X/L_Edd ~ 10^{-8}
- 10^{-7}), and colors or spectra consistent with accreting supermassive black
holes (SMBHs)--except for the nucleus of NGC 4486B, which is softer than
typical AGN spectra. In a few cases, the X-ray morphology of the nuclear
sources shows hints of marginally extended structures, in addition to the
surrounding diffuse thermal emission from hot gas, which is detectable on
scales >~ 1 kpc. In one case (NGC 5845), a dusty disk may partially obstruct
our direct view of the SMBH. We have estimated the temperature and density of
the hot interstellar medium, which is one major source of fuel for the
accreting SMBH; typical central densities are n_e ~ (0.02 +/- 0.01) cm^{-3}.
Assuming that the hot gas is captured by the SMBH at the Bondi rate, we show
that the observed X-ray luminosities are too faint to be consistent with
standard disk accretion, but brighter than predicted by radiatively-inefficient
solutions (eg, ADAF). In total, there are ~ 20 galaxies for which SMBH mass,
hot gas density, and nuclear X-ray luminosity are simultaneously known. In some
cases, the nuclear sources are brighter than predicted by the ADAF model; in
other cases, they are consistent or fainter. We discuss the apparent lack of
correlations between Bondi rate and X-ray luminosity, and suggest that, in
order to understand the observed distribution, we need to know two additional
parameters: the amount of gas supplied by the stellar population inside the
accretion radius, and the fraction (possibly << 1) of the total gas available
that is accreted by the SMBH. We shall discuss these issues in our Paper II.Comment: 18 pages, accepted by ApJ. This is Paper I; Paper II will be on
astro-ph next Monda
B,V,I - photometry of 20 dwarf irregular galaxies within 10 Mpc
CCD - photometry is presented for 20 dIrr galaxies situated in the nearby
complexes CenA/M83, and CVnI as well as in the general field of the Local
Volume. We present integrated magnitudes of the galaxies in B,V,I - bands and
also surface brightness profiles to a median isophote mu_B ~ 28 mag /sq.arcsec.
The popular Sersic parameterization of surface brightness profiles generally
does a poor job of simultaneously fitting the inner cores and outer exponential
surface brightness fall-offs observed in many of our targets. The observed
sample is a part of a general project to image about 500 nearby (D < 10 Mpc)
dwarf galaxies in multiple bands.Comment: 3 figures, accepted to the MNRA
Local galaxy flows within 5 Mpc
We present Hubble Space Telescope/WFPC2 images of sixteen dwarf galaxies as
part of our snapshot survey of nearby galaxy candidates. We derive their
distances from the luminosity of the tip of the red giant branch stars with a
typical accuracy of ~12%. The resulting distances are 4.26 Mpc (KKH 5), 4.74
Mpc (KK 16), 4.72 Mpc (KK 17), 4.66 Mpc (ESO 115-021), 4.43 Mpc (KKH 18), 3.98
Mpc (KK 27), 4.61 Mpc (KKH 34), 4.99 Mpc (KK 54), 4.23 Mpc (ESO 490-017), 4.90
Mpc (FG 202), 5.22 Mpc (UGC 3755), 5.18 Mpc (UGC 3974), 4.51 Mpc (KK 65), 5.49
Mpc (UGC 4115), 3.78 Mpc (NGC 2915), and 5.27 Mpc (NGC 6503). Based on
distances and radial velocities of 156 nearby galaxies, we plot the local
velocity-distance relation, which has a slope of H_0 = 73 km/(c * Mpc) and a
radial velocity dispersion of 85 km/s. When members of the M81 and CenA groups
are removed, and distance errors are taken into account, the radial velocity
dispersion drops to sigma_v=41 km/s. The local Hubble flow within 5 Mpc exibits
a significant anisotropy, with two infall peculiar velocity regions directed
towards the Supergalactic poles. However, two observed regions of outflow
peculiar velocity, situated on the Supergalactic equator, are far away (~50
degr.) from the Virgo/anti-Virgo direction, which disagrees with a spherically
symmetric Virgo-centric flow. About 63% of galaxies within 5 Mpc belong to
known compact and loose groups. Apart from them, we found six new probable
groups, consisting entirely of dwarf galaxies.Comment: 22 pages, 7 figures. A&A Accepted. High resolution Figures 1 and 2
(9616k) are available at http://www.sao.ru/~sme/figs.tar.g
Infrared luminosities of galaxies in the Local Volume
Near-infrared properties of 451 galaxies with distances D \leq 10 Mpc are
considered basing on the all-sky two micron survey (2MASS). A luminosity
function of the galaxies in the K-band is derived within [-25,-11] mag. The
local (D < 8 Mpc) luminosity density is estimated to be 6.8*10^8 L_sun/Mpc^3
that exceeds (1.5+-0.1) times the global cosmic density in the K-band. Virial
mass-to-K-luminosity ratios are determined for nearby groups and clusters. In
the luminosity range of (5*10^{10} - 2*10^{13})L_sun, the groups and clusters
follow the relation \lg(M/L_K) propto (0.27+-0.03) lg(L_K) with a scatter of
\~0.1 comparable to errors of the observables. The mean ratio ~=
(20-25) M_sun/L_sun for the galaxy systems turns out to be significantly lower
than the global ratio, (80-90)M_sun/L_sun, expected in the standard
cosmological model with the matter density of Omega_m =0.27. This discrepancy
can be resolved if most of dark matter in the universe is not associated with
galaxies and their systems.Comment: 15 pages, 7 figures. Astronomy Letters, submitte
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