1,031 research outputs found
An Analysis of ALMA Deep Fields and the Perceived Dearth of High-z Galaxies
Deep, pencil-beam surveys from ALMA at 1.1-1.3mm have uncovered an apparent
absence of high-redshift dusty galaxies, with existing redshift distributions
peaking around . This has led to a perceived dearth of dusty
systems at , and the conclusion, according to some models, that the early
Universe was relatively dust-poor. In this paper, we extend the backward
evolution galaxy model described by Casey et al. (2018) to the ALMA regime (in
depth and area) and determine that the measured number counts and redshift
distributions from ALMA deep field surveys are fully consistent with
constraints of the infrared luminosity function (IRLF) at determined by
single-dish submillimeter and millimeter surveys conducted on much larger
angular scales (deg). We find that measured 1.1-1.3mm number
counts are most constraining for the measurement of the faint-end slope of the
IRLF at . Recent
studies have suggested that UV-selected galaxies at may be particularly
dust-poor, but we find their millimeter-wave emission cannot rule out
consistency with the Calzetti dust attenuation law even by assuming relatively
typical, cold-dust (K) SEDs. Our models suggest that
the design of ALMA deep fields requires substantial revision to constrain the
prevalence of early Universe obscured starbursts. The most promising
avenue for detection and characterization of such early dusty galaxies will
come from future ALMA 2mm blank field surveys covering a few hundred
arcmin and the combination of existing and future dual-purpose 3mm
datasets.Comment: 21 pages, 12 figures, accepted for publication in Ap
Constraining the Lyα escape fraction with far-infrared observations of Lyα emitters
We study the far-infrared properties of 498 Lyα emitters (LAEs) at z = 2.8, 3.1, and 4.5 in the Extended Chandra Deep Field-South, using 250, 350, and 500μm data from the Herschel Multi-tiered Extragalactic Survey and 870μm data from the LABOCA ECDFS Submillimeter Survey. None of the 126, 280, or 92 LAEs at z = 2.8, 3.1, and 4.5, respectively, are individually detected in the far-infrared data. We use stacking to probe the average emission to deeper flux limits, reaching 1σ depths of ∼0.1 to 0.4 mJy. The LAEs are also undetected at ?3σ in the stacks, although a 2.5σ signal is observed at 870μm for the z = 2.8 sources. We consider a wide range of far-infrared spectral energy distributions (SEDs), including an M82 and an Sd galaxy template, to determine upper limits on the far-infrared luminosities and far-infrared-derived star formation rates of the LAEs. These star formation rates are then combined with those inferred from the Lyα and UV emission to determine lower limits on the LAEs’ Lyα escape fraction (f esc (Lyα)). For the Sd SED template, the inferred LAEs f esc (Lyα) are ?30% (1σ) at z = 2.8, 3.1, and 4.5, which are all significantly higher than the global f esc (Lyα) at these redshifts. Thus, if the LAEs f esc (Lyα) follows the global evolution, then they have warmer far-infrared SEDs than the Sd galaxy template. The average and M82 SEDs produce lower limits on the LAE f esc (Lyα) of ∼10%–20% (1σ), all of which are slightly higher than the global evolution of f esc (Lyα), but consistent with it at the 2σ–3σ level
Effects of Star Formation Stochasticity on the Ly-alpha & Lyman Continuum Emission from Dwarf Galaxies during Reionization
Observations of distant galaxies play a key role in improving our
understanding of the Epoch of Reionization (EoR). The observed Ly-alpha
emission line strength - quantified by its restframe equivalent width (EW) -
provides a valuable diagnostic of stellar populations and dust in galaxies
during and after the EoR. In this paper we quantify the effects of star
formation stochasticity on the predicted Ly-alpha EW in dwarf galaxies, using
the publicly available code SLUG ('Stochastically Light Up Galaxies'). We
compute the number of hydrogen ionizing photons, as well as flux in the Far UV
for a set of models with star formation rates (SFR) in the range 10-3-1
Msol/yr. From these fluxes we compute the luminosity, L-alpha, and the EW of
the Ly-alpha line. We find that stochasticity alone induces a broad
distribution in L-alpha and EW at a fixed SFR, and that the widths of these
distributions decrease with increasing SFR. We parameterize the EW probability
density function (PDF) as an SFR-dependent double power law. We find that it is
possible to have EW as low as ~EW0/4 and as high as ~3 times the EW0, where EW0
denotes the expected EW in the absence of stochasticity. We argue that
stochasticity may therefore be important when linking drop-out and narrow-band
selected galaxies, when identifying population III galaxies, and that it may
help to explain the large EW (EW > 100 - 200 A) observed for a fraction of
Ly-alpha- selected galaxies. Finally, we show that stochasticity can also
affect the inferred escape fraction of ionizing photons from galaxies. In
particular, we argue that stochasticity may simultaneously explain the observed
anomalous ratios of the Lyman continuum flux density to the (non-ionizing) UV
continuum density in so-called Lyman-Bump galaxies at z = 3.1, as well as the
absence of such objects among a sample of z = 1.3 drop-out galaxies.Comment: 9 pages, 4 figures, accepted for publication in MNRA
The Brightest Galaxies in the Dark Ages: Galaxies' Dust Continuum Emission During the Reionization Era
Though half of cosmic starlight is absorbed by dust and reradiated at long
wavelengths (3m-3mm), constraints on the infrared through millimeter
galaxy luminosity function (the `IRLF') are poor in comparison to the
rest-frame ultraviolet and optical galaxy luminosity function, particularly at
z>2.5. Here we present a backward evolution model for interpreting number
counts, redshift distributions, and cross-band flux density correlations in the
infrared and submillimeter sky, from 70m-2mm, using a model for the IRLF
out to the epoch of reionization. Mock submillimeter maps are generated by
injecting sources according to the prescribed IRLF and flux densities drawn
from model spectral energy distributions that mirror the distribution of SEDs
observed in dusty star-forming galaxies (DSFGs). We explore two extreme
hypothetical case-studies: a dust-poor early Universe model, where DSFGs
contribute negligibly (10%) to the integrated star-formation rate density at
, and an alternate dust-rich early Universe model, where DSFGs dominate
90% of star-formation. We find that current submm/mm datasets do
not clearly rule out either of these extreme models. We suggest that future
surveys at 2mm will be crucial to measuring the IRLF beyond . The model
framework developed in this paper serves as a unique tool for the
interpretation of multiwavelength IR/submm extragalactic datasets and will
enable more refined constraints on the IRLF than can be made from direct
measurements of individual galaxies' integrated dust emission.Comment: 34 pages, 16 figures, accepted for publication in Ap
At the crossroads of biomacromolecular research: highlighting the interdisciplinary nature of the field
Due to their complexity and wide-ranging utility, biomacromolecular research is an especially interdisciplinary branch of chemistry. It is my goal that the Biomacromolecules subject area of Chemistry Central Journal will parallel this richness and diversity. In this inaugural commentary, I attempt to set the stage for achieving this by highlighting several areas where biomacromolecular research overlaps more traditional chemistry sub-disciplines. Specifically, it is discussed how Materials Science and Biotechnology, Analytical Chemistry, Cell Biology and Chemical Theory are each integral to modern biomacromolecular research. Investigators with reports in any of these areas, or any other dealing with biomacromolecules, are encouraged to submit their research papers to Chemistry Central Journal
Nucleon Form Factors from 5D Skyrmions
Several aspects of hadron physics are well described by a simple 5D effective
field theory. Baryons arise in this scenario as "large" (and therefore
calculable) 5D skyrmions. We extend and refine the existing analysis of this 5D
soliton, which is fairly non-trivial due to the need of numerical methods. We
perform the complete quantization of those collective coordinates which are
relevant for computing the static observables like the nucleon form factors. We
compare the result with simple expectations about large-N_c QCD and with the
experimental data. An agreement within 30% is found.Comment: 30 pages, 6 figures; v2: References added and typos corrected; v3:
Version published in Nucl. Phys.
A low-voltage activated, transient calcium current is responsible for the time-dependent depolarizing inward rectification of rat neocortical neurons in vitro
Intracellular recordings were obtained from rat neocortical neurons in vitro. The current-voltage-relationship of the neuronal membrane was investigated using current- and single-electrode-voltage-clamp techniques. Within the potential range up to 25 mV positive to the resting membrane potential (RMP: –75 to –80 mV) the steady state slope resistance increased with depolarization (i.e. steady state inward rectification in depolarizing direction). Replacement of extracellular NaCl with an equimolar amount of choline chloride resulted in the conversion of the steady state inward rectification to an outward rectification, suggesting the presence of a voltage-dependent, persistent sodium current which generated the steady state inward rectification of these neurons. Intracellularly injected outward current pulses with just subthreshold intensities elicited a transient depolarizing potential which invariably triggered the first action potential upon an increase in current strength. Single-electrode-voltage-clamp measurements reveled that this depolarizing potential was produced by a transient calcium current activated at membrane potentials 15–20 mV positive to the RMP and that this current was responsible for the time-dependent increase in the magnitude of the inward rectification in depolarizing direction in rat neocortical neurons. It may be that, together with the persistent sodium current, this calcium current regulates the excitability of these neurons via the adjustment of the action potential threshold
A massive, quiescent galaxy at redshift of z=3.717
In the early Universe finding massive galaxies that have stopped forming
stars present an observational challenge as their rest-frame ultraviolet
emission is negligible and they can only be reliably identified by extremely
deep near-infrared surveys. These have revealed the presence of massive,
quiescent early-type galaxies appearing in the universe as early as z2,
an epoch 3 Gyr after the Big Bang. Their age and formation processes have now
been explained by an improved generation of galaxy formation models where they
form rapidly at z3-4, consistent with the typical masses and ages derived
from their observations. Deeper surveys have now reported evidence for
populations of massive, quiescent galaxies at even higher redshifts and earlier
times, however the evidence for their existence, and redshift, has relied
entirely on coarsely sampled photometry. These early massive, quiescent
galaxies are not predicted by the latest generation of theoretical models.
Here, we report the spectroscopic confirmation of one of these galaxies at
redshift z=3.717 with a stellar mass of 1.710 M whose
absorption line spectrum shows no current star-formation and which has a
derived age of nearly half the age of the Universe at this redshift. The
observations demonstrates that the galaxy must have quickly formed the majority
of its stars within the first billion years of cosmic history in an extreme and
short starburst. This ancestral event is similar to those starting to be found
by sub-mm wavelength surveys pointing to a possible connection between these
two populations. Early formation of such massive systems is likely to require
significant revisions to our picture of early galaxy assembly.Comment: 6 pages, 7 figures. This is the final preprint corresponding closely
to the published version. Uploaded 6 months after publication in accordance
with Nature polic
Bi-local Construction of Sp(2N)/dS Higher Spin Correspondence
We derive a collective field theory of the singlet sector of the Sp(2N) sigma
model. Interestingly the hamiltonian for the bilocal collective field is the
same as that of the O(N) model. However, the large-N saddle points of the two
models differ by a sign. This leads to a fluctuation hamiltonian with a
negative quadratic term and alternating signs in the nonlinear terms which
correctly reproduces the correlation functions of the singlet sector. Assuming
the validity of the connection between O(N) collective fields and higher spin
fields in AdS, we argue that a natural interpretation of this theory is by a
double analytic continuation, leading to the dS/CFT correspondence proposed by
Anninos, Hartman and Strominger. The bi-local construction gives a map into the
bulk of de Sitter space-time. Its geometric pseudospin-representation provides
a framework for quantization and definition of the Hilbert space. We argue that
this is consistent with finite N grassmanian constraints, establishing the
bi-local representation as a nonperturbative framework for quantization of
Higher Spin Gravity in de Sitter space.Comment: 1 figur
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