1,371 research outputs found
The Lyman Break Galaxies: their Progenitors and Descendants
We study the evolution of Lyman Break Galaxies (LBGs) from z=5 to z=0 by
tracing the merger trees of galaxies in a large-scale hydrodynamic simulation
based on a Lambda cold dark matter model. In particular, we emphasize on the
range of properties of the sample selected by the rest-frame V band luminosity,
in accordance with recent near-IR observations. The predicted rest-frame V band
luminosity function agrees well with the observed one when dust extinction is
taken into account. The stellar content and the star formation histories of
LBGs are also studied. We find that the LBGs intrinsically brighter than
Mv=-21.0 at z=3 have stellar masses of at least 10^9\Msun, with a median of
10^{10}h^{-1}\Msun. The brightest LBGs (Mv<-23) at z=3 merge into
clusters/groups of galaxies at z=0, as suggested from clustering studies of
LBGs. Roughly one half of the galaxies with -23<Mv<-22 at z=3 fall into
groups/clusters, and the other half become typical L* galaxies at z=0 with
stellar mass of ~10^{11}\Msun. Descendants of LBGs at the present epoch have
formed roughly 30% of their stellar mass by z=3, and the half of their current
stellar population is 10 Gyr old, favoring the scenario that LBGs are the
precursors of the present day spheroids. We find that the most luminous LBGs
have experienced a starburst within 500 Myr prior to z=3, but also have formed
stars continuously over a period of 1 Gyr prior to z=3 when all the star
formation in progenitors is coadded. We also study the evolution of the mean
stellar metallicity distribution of galaxies, and find that the entire
distribution shifts to lower metallicity at higher redshift. The observed
sub-solar metallicity of LBGs at z=3 is naturally predicted in our simulation.Comment: 29 pages, including 11 figures, ApJ in press. One reference adde
Distribution of Damped Lyman-alpha Absorbers in a Lambda Cold Dark Matter Universe
We present the results of a numerical study of a galactic wind model and its
implications on the properties of damped Lyman-alpha absorbers (DLAs) using
cosmological hydrodynamic simulations. We vary both the wind strength and the
internal parameters of the the wind model in a series of cosmological SPH
simulations that include radiative cooling and heating by a UV background, star
formation, and feedback from supernovae and galactic winds. To test our
simulations, we examine the DLA `rate-of-incidence' as a function of halo mass,
galaxy apparent magnitude, and impact parameter. We find that the statistical
distribution of DLAs does not depend on the exact values of internal numerical
parameters that control the decoupling of hydrodynamic forces when the gas is
ejected from starforming regions. The DLA rate-of-incidence in our simulations
at z=3 is dominated by the faint galaxies with apparent magnitude R_AB < 25.5.
However, interestingly in a `strong wind' run, the differential distribution of
DLA sight-lines is peaked at Mhalo = 10^{12} Msun/h (R_AB~27), and the mean DLA
halo mass is Mmean=10^{12.4} Msun/h (R_AB ~ 26). These mass-scales are much
larger than those if we ignore winds, because galactic wind feedback suppresses
the DLA cross section in low-mass halos and increases the relative contribution
to the DLA incidence from more massive halos. The DLAs in our simulations are
more compact than the present-day disk galaxies, and the impact parameter
distribution is very narrow unless we limit the search for the host galaxy to
only bright LBGs. The comoving number density of DLAs is higher than that of
LBGs down to R_AB=30 mag if the physical radius of each DLA is smaller than 5
kpc/h_70. We discuss conflicts between current simulations and observations,
and potential problems with simulations based on the CDM model.Comment: 37 pages, 11 figures. Accepted to ApJ. Additional numerical tests of
the internal parameters of the galactic wind model are presente
Massive galaxies in cosmological simulations: UV-selected sample at redshift z=2
We study the properties of galaxies at z=2 in a Lambda CDM universe, using
two different types of hydrodynamic simulation methods (Eulerian TVD and SPH)
and a spectrophotometric analysis in the Un, G, R filter set. The simulated
galaxies at z=2 satisfy the color-selection criteria proposed by Adelberger et
al. (2004) when we assume Calzetti extinction with E(B-V)=0.15. We find that
the number density of simulated galaxies brighter than R<25.5 at z=2 is about
2e-2 h^3/Mpc^3, roughly one order of magnitude larger than that of Lyman break
galaxies at z=3. The most massive galaxies at z=2 have stellar masses >~1e11
Msun, and their observed-frame G-R colors lie in the range 0.0<G-R<1.0. They
typically have been continuously forming stars with a rate exceeding 30 Msun/yr
over a few Gyrs from z=10 to z=2, although the TVD simulation indicates a more
sporadic star formation history than the SPH simulations. Of order half of
their stellar mass was already assembled by z~4. The reddest massive galaxies
at z=2 with G-R >= 1.0 and Mstar>1e10 Msun/h finished the build-up of their
stellar mass by z~3. Interestingly, our study suggests that the majority of the
most massive galaxies at z=2 should be detectable at rest-frame UV wavelengths,
contrary to some recent claims made on the basis of near-IR studies of galaxies
at the same epoch, provided the median extinction is less than E(B-V)<0.3.
However, our results also suggest that the fraction of stellar mass contained
in galaxies that pass the color-selection criteria could be as low as 50% of
the total stellar mass in the Universe at z=2. Our simulations suggest that the
missing stellar mass is contained in fainter (R>25.5) and intrinsically redder
galaxies. Our results do not suggest that hierarchical galaxy formation fails
to account for the massive galaxies at z>=1. (abridged)Comment: 35 pages, 11 figures. Submitted to ApJ. Error in AB magnitude
calculation corrected. Higher resolution version available at
http://cfa-www.harvard.edu/~knagamine/redgal.ps.g
Hyperfine Populations Prior to Muon Capture
It is shown that the 1S level hyperfine populations prior to muon capture
will be statistical when either target or beam are unpolarised independent of
the atomic level at which the hyperfine interaction becomes appreciable. This
assertion holds in the absence of magnetic transitions during the cascade and
is true because of minimal polarisation after atomic capture and selective
feeding during the cascade.Comment: (revtex, 6 preprint pages, no figures
Detectability of [CII] 158 micron emission from high-redshift galaxies: predictions for ALMA and SPICA
We discuss the detectability of high-redshift galaxies via [CII] 158 micron
line emission by coupling an analytic model with cosmological Smoothed Particle
Hydrodynamics (SPH) simulations that are based on the concordance Lambda cold
dark matter (CDM) model. Our analytic model describes a multiphase interstellar
medium irradiated by the far ultra-violet radiation from local star-forming
regions, and it calculates thermal and ionization equilibrium between cooling
and heating. The model allows us to predict the mass fraction of a cold neutral
medium (CNM) embedded in a warm neutral medium (WNM). Our cosmological SPH
simulations include a treatment of radiative cooling/heating, star formation,
and feedback effects from supernovae and galactic winds. Using our method, we
make predictions for the [CII] luminosity from high-redshift galaxies which can
be directly compared with upcoming observations by the Atacama Large Millimeter
Array (ALMA) and the Space Infrared Telescope for Cosmology and Astrophysics
(SPICA). We find that the number density of high-redshift galaxies detectable
by ALMA and SPICA via [CII] emission depends significantly on the amount of
neutral gas which is highly uncertain. Our calculations suggest that, in a CDM
universe, most [CII] sources at z=3 are faint objects with \Snu < 0.01 mJy.
Lyman-break galaxies (LBGs) brighter than R_AB=23.5 mag are expected to have
flux densities \Snu = 1-3 mJy depending on the strength of galactic wind
feedback. The recommended observing strategy for ALMA and SPICA is to aim at
very bright LBGs or star-forming DRG/BzK galaxies.Comment: 39 pages, 13 figures, accepted to ApJ. Matched to the accepted
versio
Imaging the cool gas, dust, star formation, and AGN in the first galaxies
When, and how, did the first galaxies and supermassive black holes (SMBH)
form, and how did they reionization the Universe? First galaxy formation and
cosmic reionization are among the last frontiers in studies of cosmic structure
formation. We delineate the detailed astrophysical probes of early galaxy and
SMBH formation afforded by observations at centimeter through submillimeter
wavelengths. These observations include studies of the molecular gas (= the
fuel for star formation in galaxies), atomic fine structure lines (= the
dominant ISM gas coolant), thermal dust continuum emission (= an ideal star
formation rate estimator), and radio continuum emission from star formation and
relativistic jets. High resolution spectroscopic imaging can be used to study
galaxy dynamics and star formation on sub-kpc scales. These cm and mm
observations are the necessary compliment to near-IR observations, which probe
the stars and ionized gas, and X-ray observations, which reveal the AGN.
Together, a suite of revolutionary observatories planned for the next decade
from centimeter to X-ray wavelengths will provide the requisite panchromatic
view of the complex processes involved in the formation of the first generation
of galaxies and SMBHs, and cosmic reionization.Comment: 8 pages total. White paper submitted to the Astro 2010 Decadal Surve
Tuning the antiferromagnetic easy axis direction in exchange bias bilayers
Abstract The exchange bias effect is measured for a Co/NiO bilayer before and after it has been cooled down from 580 K in 1.5 kOe magnetic field applied at 45 to the initial exchange-bias direction. The angular variation of the hysteresis loop shift for the treated sample showed three distinct minima and maxima, in contrast to that of the as-made sample, which is characteristic for a system with aligned ferromagnetic and antiferromagnetic easy axes. This behavior is qualitatively well explained in the framework of the domain-wall formation model applied for the off-aligned case. The continued interest in the exchange-bias effect, which results from the interfacial coupling between ferromagnetic (FM) and antiferromagnetic (AF) materials, is motivated by fundamental and technological interests. In almost all of the model works, the direction of the easy axis of the AF layer is aligned with the FM one; some numerical calculations using a simple StonerWohlfarth model for the case of ''off-aligned'' coupling have been done by Xi and White In the present work, a FM/AF bilayer was deposited by magnetron sputtering onto Si(1 0 0) substrate at room temperature (RT) in 2.0 mTorr Ar atmosphere with base pressure before depositing better than 5 Ă 10 Ă8 Torr. The film consists of 30 nm Co deposited on 50 nm NiO and capped with 5 nm Cu in order to prevent oxidation in air. Magnetic field of 0.5 kOe has been applied during the deposition. The structural characterization, made via conventional X-ray diffractometry performed on a Philips X'Pert MRD machine employing Cu Ka radiation, showed that the Co layer is strongly (2 2 0) textured, whereas the NiO contribution is a combination of evenly divided (1 1 1) and (2 0 0) NiO textures. In-plane RT hysteresis loops were obtained by using an alternating gradient force magnetometer. No training effect, i.e., dependence of the hysteresis loop field shift, H eb ; on repeated magnetization reversal, has been observed. The sample was heated to 580 K, which is higher than the NiO N! eel temperature of 520 K but rather lower than the Curie temperature of Co, and then cooled down to RT in the presence of a magnetic field of 1.5 kOe applied at 45 (75) to the initial exchange-bias direction. Once again, effects of training have not been detected
The K20 survey. VI. The Distribution of the Stellar Masses in Galaxies up to z~2
We present a detailed analysis of the stellar mass content of galaxies up to
z=2.5 in the K20 galaxy sample, that has a 92% spectroscopic completeness and a
complete multicolor coverage. We find that the M/L ratio decreases
with redshift: in particular, the average M/L ratio of early type galaxies
decreases with , with a scatter that is indicative of a range of
star--formation time-scales and redshift of formation. More important, the
typical M/L of massive early type galaxies is larger than that of less massive
ones, suggesting that their stellar population formed at higher z. The final
K20 galaxy sample spans a range of stellar masses from M*=10^9Msun to
M*=10^12Msun, with massive galaxies ($M*>10^11Msun) detected up to z~2. We
compute the Galaxy Stellar Mass Function at various z, of which we observe only
a mild evolution (i.e. by 20-30%) up to z~1. At z>1, the evolution of the GSMF
appears to be much faster: at z~2, about 35% of the present day stellar mass in
objects with M*~10^11Msun appear to have assembled. We also detect a change in
the physical nature of the most massive galaxies, since at z>1 a population of
massive star--forming galaxies progressively appears. We finally analyze our
results in the framework of Lambda-CDM hierarchical models. First, we show that
the large number of massive galaxies detected at high z does not violate any
fundamental Lambda-CDM constraint based on the number of massive DM halos.
Then, we compare our results with the predictions of renditions of both
semianalytic and hydro-dynamical models, that range from severe underestimates
to slight overestimates of the observed mass density at z<~2. We discuss how
the differences among these models are due to the different implementation of
the main physical processes. (Abridged)Comment: Accepted for publication on Astronomy & Astrophysic
A new measurement of the evolving near-infrared galaxy luminosity function out to z~4: a continuing challenge to theoretical models of galaxy formation
We present the most accurate measurement to date of cosmological evolution of
the near-infrared galaxy luminosity function, from the local Universe out to
z~4. The analysis is based on a large and highly complete sample of galaxies
selected from the first data release of the UKIDSS Ultra Deep Survey.
Exploiting a master catalogue of K- and z-band selected galaxies over an area
of 0.7 square degrees, we analyse a sample of ~50,000 galaxies, all with
reliable photometry in 16-bands from the far-ultraviolet to the mid-infrared.
The unique combination of large area and depth provided by the Ultra Deep
Survey allows us to trace the evolution of the K-band luminosity function with
unprecedented accuracy. In particular, via a maximum likelihood analysis we
obtain a simple parameterization for the luminosity function and its
cosmological evolution, including both luminosity and density evolution, which
provides an excellent description of the data from z =0 up to z~4. We find
differential evolution for galaxies dependent on galaxy luminosity, revealing
once again the ``down-sizing behaviour'' of galaxy formation. Finally, we
compare our results with the predictions of the latest theoretical models of
galaxy formation, based both on semi-analytical prescriptions, and on full
hydrodynamical simulations.Comment: 11 pages, 6 figures, submitted to MNRA
The First Cold Antihydrogen
Antihydrogen, the atomic bound state of an antiproton and a positron, was
produced at low energy for the first time by the ATHENA experiment, marking an
important first step for precision studies of atomic antimatter. This paper
describes the first production and some subsequent developments.Comment: Invitated Talk at COOL03, International Workshop on Beam Cooling and
Related Topics, to be published in NIM
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