3,762 research outputs found
Emission Line Galaxies in the STIS Parallel Survey II: Star Formation Density
We present the luminosity function of [OII]-emitting galaxies at a median
redshift of z=0.9, as measured in the deep spectroscopic data in the STIS
Parallel Survey (SPS). The luminosity function shows strong evolution from the
local value, as expected. By using random lines of sight, the SPS measurement
complements previous deep single field studies. We calculate the density of
inferred star formation at this redshift by converting from [OII] to H-alpha
line flux as a function of absolute magnitude and find rho_dot=0.043 +/- 0.014
Msun/yr/Mpc^3 at a median redshift z~0.9 within the range 0.46<z<1.415 (H_0 =
70 km/s/Mpc, Omega_M=0.3, Omega_Lambda=0.7. This density is consistent with a
(1+z)^4 evolution in global star formation since z~1. To reconcile the density
with similar measurements made by surveys targeting H-alpha may require
substantial extinction correction.Comment: 16 preprint pages including 5 figures; accepted for publication in
Ap
Machines Versus Humans: The Counting and Recounting of Pre-Scored Punchcard Ballots
The counting of ballots, especially punchcard ballots, has received a great deal of attention in the years following the 2000 presidential election in Florida. Much of the research literature has focused on various measures of how accurately voting machines record voter intentions, with studies of the relative accuracy rates across voting machines (e.g., Caltech/MIT Voting Technology Project 2001), studies of voting accuracy across groups of the electorate (Alvarez and Sinclair 2003), and studies that examine the variability in voting machine accuracy across both machine types and voter types (Alvarez, Sinclair and Wilson 2002; Ansolabehere 2002; Tomz and Van Houweling 2003).Carnegie Corporation of New York; John S. and James L. Knight Foundation; John Randolph Haynes and Dora Haynes Foundatio
Measurements of the Diffuse Ultraviolet Background and the Terrestrial Airglow with the Space Telescope Imaging Spectrograph
Far-UV observations in and near the Hubble Deep Fields demonstrate that the
Space Telescope Imaging Spectrograph (STIS) can potentially obtain unique and
precise measurements of the diffuse far-ultraviolet background. Although STIS
is not the ideal instrument for such measurements, high-resolution images allow
Galactic and extragalactic objects to be masked to very faint magnitudes, thus
ensuring a measurement of the truly diffuse UV signal. The programs we have
analyzed were not designed for this scientific purpose, but would be sufficient
to obtain a very sensitive measurement if it were not for a weak but
larger-than-expected signal from airglow in the STIS 1450-1900 A bandpass. Our
analysis shows that STIS far-UV crystal quartz observations taken near the limb
during orbital day can detect a faint airglow signal, most likely from NI\1493,
that is comparable to the dark rate and inseparable from the far-UV background.
Discarding all but the night data from these datasets gives a diffuse
far-ultraviolet background measurement of 501 +/- 103 ph/cm2/sec/ster/A, along
a line of sight with very low Galactic neutral hydrogen column (N_HI = 1.5E20
cm-2) and extinction (E(B-V)=0.01 mag). This result is in good agreement with
earlier measurements of the far-UV background, and should not include any
significant contribution from airglow. We present our findings as a warning to
other groups who may use the STIS far-UV camera to observe faint extended
targets, and to demonstrate how this measurement may be properly obtained with
STIS.Comment: 7 pages, Latex. 4 figures. Uses corrected version of emulateapj.sty
and apjfonts.sty (included). Accepted for publication in A
A simplified model for minor and major loop magnetic hysteresis and its application for inference of temperature in induction heated particle beds
In this work, a LangArc model is presented that successfully fits both major and minor hysteresis loops of a bed of magnetic particles in real time using instruments that detect changes in the magnetic field strength, such as in-situ pick-up coils. A novel temperature measurement application is demonstrated based on a real-time characterisation of a magnetic material, in this case magnetite, as a function of temperature. Magnetic hysteresis can be used to provide useful induction heating in a packed bed of magnetic materials. This can be used for general heating and to provide energy to chemical reactions in chemical processes. Accurate temperature measurement of magnetic particles under induction heating is a well-known challenge: conventional techniques give a single-point measurement, and are subject to inaccuracy due to self-heating of the instrument tip. Thermal lag can be problematic given the rapid heating rates that are characteristic of induction heating. The LangArc inferred temperature measurement technique is shown to detect heating rates in excess of 30 °C·sâ1, under which circumstances an in-bed thermocouple was shown to lag by as much as 180 °C. This new method has significant importance for temperature measurement in applications involving the induction heating of magnetic materials as it avoids the location of an instrument inside the magnetic particle bed and is highly responsive under rapid heating where other techniques can give misleading results.</p
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Characterization of the fecal microbiome in cats with inflammatory bowel disease or alimentary small cell lymphoma.
Feline chronic enteropathy (CE) is a common gastrointestinal disorder in cats and mainly comprises inflammatory bowel disease (IBD) and small cell lymphoma (SCL). Both IBD and SCL in cats share features with chronic enteropathies such as IBD and monomorphic epitheliotropic intestinal T-cell lymphoma in humans. The aim of this study was to characterize the fecal microbiome of 38 healthy cats and 27 cats with CE (13 cats with IBD and 14 cats with SCL). Alpha diversity indices were significantly decreased in cats with CE (OTU pâ=â0.003, Shannon Index pâ=â0.008, Phylogenetic Diversity pâ=â0.019). ANOSIM showed a significant difference in bacterial communities, albeit with a small effect size (Pâ=â0.023, Râ=â0.073). Univariate analysis and LEfSE showed a lower abundance of facultative anaerobic taxa of the phyla Firmicutes (families Ruminococcaceae and Turicibacteraceae), Actinobacteria (genus Bifidobacterium) and Bacteroidetes (i.a. Bacteroides plebeius) in cats with CE. The facultative anaerobic taxa Enterobacteriaceae and Streptococcaceae were increased in cats with CE. No significant difference between the microbiome of cats with IBD and those with SCL was found. Cats with CE showed patterns of dysbiosis similar to those in found people with IBD
Parallélisation et optimisation d'un simulateur de morphogénÚse d'organes. Application aux éléments du rein
Depuis plusieurs dizaines d annĂ©es, la modĂ©lisation du vivant est un enjeu majeur qui nĂ©cessite de plus en plus de travaux dans le domaine de la simulation. En effet, elle ouvre la porte Ă toute une palette d applications: l aide Ă la dĂ©cision en environnement et en Ă©cologie, l aide Ă l enseignement, l aide Ă la dĂ©cision pour les mĂ©decins, l aide Ă la recherche de nouveaux traitements pharmaceutiques et la biologie dite prĂ©dictive , etc. Avant de pouvoir aborder un problĂšme, il est nĂ©cessaire de pouvoir modĂ©liser de façon prĂ©cise le systĂšme biologique concernĂ© en prĂ©cisant bien les questions auxquelles devra rĂ©pondre le modĂšle. La manipulation et l Ă©tude de systĂšmes complexes, les systĂšmes biologiques en Ă©tant l archĂ©type, pose, de façon gĂ©nĂ©rale, des problĂšmes de modĂ©lisation et de simulation. C est dans ce contexte que la sociĂ©tĂ© Integrative BioComputing (IBC) dĂ©veloppe depuis le dĂ©but des annĂ©es 2000 un prototype d une Plateforme GĂ©nĂ©rique de ModĂ©lisation et de Simulation(la PGMS) dont le but est de fournir un environnement pour modĂ©liser et simuler plus simplement les processus et les fonctions biologiques d un organisme complet avec les organes le composant. La PGMS Ă©tant une plateforme gĂ©nĂ©rique encore en phase de dĂ©veloppement, elle ne possĂ©dait pas les performances nĂ©cessaires pour permettre de rĂ©aliser la modĂ©lisation et la simulation d Ă©lĂ©ments importants dans des temps suffisamment courts. Il a donc Ă©tĂ© dĂ©cidĂ©, afin d amĂ©liorer drastiquement les performances de la PGMS, de parallĂ©liser et d optimiser l implĂ©mentation de celle-ci; le but Ă©tant de permettre la modĂ©lisation et la simulation d organes complets dans des temps acceptables. Le travail rĂ©alisĂ© au cours de cette thĂšse a donc consistĂ© Ă traiter diffĂ©rents aspects de la modĂ©lisation et de la simulation de systĂšmes biologiques afin d accĂ©lĂ©rer les traitements de ceux-ci. Le traitement le plus gourmand en termes de temps de calcul lors de l exĂ©cution de la PGMS, le calcul des champs physicochimiques, a ainsi fait l objet d une Ă©tude de faisabilitĂ© de sa parallĂ©lisation. Parmi les diffĂ©rentes architectures disponibles pour parallĂ©liser une telle application, notre choix s est portĂ© sur l utilisation de GPU (Graphical Processing Unit) Ă des fins de calculs gĂ©nĂ©ralistes aussi couramment appelĂ© GPGPU (General-Purpose computation on Graphics Processing Units). Ce choix a Ă©tĂ© rĂ©alisĂ© du fait, entre autres, du coĂ»t rĂ©duit du matĂ©riel et de sa trĂšs grande puissance de calcul brute qui en fait une des architectures de parallĂ©lisation les plus accessibles du marchĂ©. Les rĂ©sultats de l Ă©tude de faisabilitĂ© Ă©tant particuliĂšrement concluant, la parallĂ©lisation du calcul des champs a ensuite Ă©tĂ© intĂ©grĂ©e Ă la PGMS. En parallĂšle, nous avons Ă©galement menĂ© des travaux d optimisations pour amĂ©liorer les performances sĂ©quentielles de la PGMS. Le rĂ©sultat de ces travaux est une augmentation de la vitesse d exĂ©cution d un facteur 18,12x sur les simulations les plus longues (passant de 16 minutes pour la simulation non optimisĂ©e utilisant un seul cĆur CPU Ă 53 secondes pour la version optimisĂ©e utilisant toujours un seul cĆur CPU mais aussi un GPU GTX500). L autre aspect majeur traitĂ© dans ces travaux a Ă©tĂ© d amĂ©liorer les performances algorithmiques pour la simulation d automates cellulaires en trois dimensions. En effet, ces derniers permettent aussi bien de simuler des comportements biologiques que d implĂ©menter des mĂ©canismes de modĂ©lisation tels que les interactions multi-Ă©chelles. Le travail de recherche s est essentiellement effectuĂ© sur des propositions algorithmiques originales afin d amĂ©liorer les simulations rĂ©alisĂ©es par IBC sur la PGMS. L accĂ©lĂ©ration logicielle, Ă travers l implĂ©mentation de l algorithme Hash Life en trois dimensions, et la parallĂ©lisation Ă l aide de GPGPU ont Ă©tĂ© Ă©tudiĂ©es de façon concomitante et ont abouti Ă des gains trĂšs significatifs en temps de calcul.For some years, living matter modeling has been a major challenge which needs more and more research in the simulation field. Indeed, the use of models of living matter have multiple applications: decision making aid in environment or ecology, teaching tools, decision making aid for physician, research aid for new pharmaceutical treatment and predictive biology, etc. But before being able to tackle all these issues, the development of a correct model, able to give answer about specific questions, is needed. Working with complex systems biologic system being the archetype of them raises various modeling and simulation issues. It is in this context that the Integrative BioComputing (IBC) company have been elaborating, since the early 2000s, the prototype of a generic platform for modeling and simulation (PGMS). Its goal is to provide a platform used to easily model and simulate biological process of a full organism, including its organs. Since the PGMS was still in its development stage at the start of my PhD, the application performance prevented the modeling and simulation of large biological components in an acceptable time. Therefore, it has been decide to optimize and parallelize its computation to increase significantly the PGMS performances. The goal was to enable the use of the PGMS to model and simulate full organs in acceptable times. During my PhD, I had to work on various aspects of the modeling and simulation of biological systems to increase their process speed. Since the most costly process during the PGMS execution was the computation of chemical fields, I had to study the opportunity of parallelizing this process. Among the various hardware architectures available to parallelize this application, we chose to use graphical processing units for general purpose computation (GPGPUs). This choice was motivated, beside other reasons, by the low cost of the hardware compared to its massive computation power, making it one of the most affordable parallel architecture on the market. Since the results of the initial feasibility study were conclusive, the parallelization of the fields computation has been integrated into the PGMS. In parallel to this work, I also worked on optimizing the sequential performance of the application. All these works lead to an increase of the software performances achieving a speed-up of 18.12x for the longest simulation (from 16 minutes for the non-optimized version with one CPU core to 53 seconds for the optimized version, still using only one core on the CPU but also a GPU GTX500). The other major aspect of my work was to increase the algorithmic performances for the simulation of three-dimensional cellular automata. In fact, these automata allow the simulation of biological behavior as they can be used to implement various mechanisms of a model such as multi-scale interactions. The research work consisted mainly in proposing original algorithms to improve the simulation provided by IBC on the PGMS. The sequential speed increase, thanks to the three-dimensional Hash Life implementation, and the parallelization on GPGPU has been studied together and achieved major computation time improvement.CLERMONT FD-Bib.Ă©lectronique (631139902) / SudocSudocFranceF
Corticosterone Acts in the Nucleus Accumbens to Enhance Dopamine Signaling and Potentiate Reinstatement of Cocaine Seeking
Stressful life events are important contributors to relapse in recovering cocaine addicts, but the mechanisms by which they influence motivational systems are poorly understood. Studies suggest that stress may âset the stageâ for relapse by increasing the sensitivity of brain reward circuits to drug-associated stimuli. We examined the effects of stress and corticosterone on behavioral and neurochemical responses of rats to a cocaine prime after cocaine self-administration and extinction. Exposure of rats to acute electric footshock stress did not by itself reinstate drug-seeking behavior but potentiated reinstatement in response to a subthreshold dose of cocaine. This effect of stress was not observed in adrenalectomized animals, and was reproduced in nonstressed animals by administration of corticosterone at a dose that reproduced stress-induced plasma levels. Pretreatment with the glucocorticoid receptor antagonist RU38486 did not block the corticosterone effect. Corticosterone potentiated cocaine-induced increases in extracellular dopamine in the nucleus accumbens (NAc), and pharmacological blockade of NAc dopamine receptors blocked corticosterone-induced potentiation of reinstatement. Intra-accumbens administration of corticosterone reproduced the behavioral effects of stress and systemic corticosterone. Corticosterone treatment acutely decreased NAc dopamine clearance measured by fast-scan cyclic voltammetry, suggesting that inhibition of uptake2-mediated dopamine clearance may underlie corticosterone effects. Consistent with this hypothesis, intra-accumbens administration of the uptake2 inhibitor normetanephrine potentiated cocaine-induced reinstatement. Expression of organic cation transporter 3, a corticosterone-sensitive uptake2 transporter, was detected on NAc neurons. These findings reveal a novel mechanism by which stress hormones can rapidly regulate dopamine signaling and contribute to the impact of stress on drug intake
Properties of Low-Lying Heavy-Light Mesons
We present preliminary results for the B meson decay constant and masses of
low-lying heavy-light mesons in the static limit. Calculations were performed
on the lattice in the quenched approximation using multistate smearing
functions generated from a Hamiltonian for a spinless relativistic quark. The
2S--1S and 1P--1S mass splittings are measured. Using the 1P--1S charmonium
splitting to set the overall scale, the ground state decay constant, f_B, is
319 +- 11 (stat) MeV.Comment: 8 pages, 9 figures, UCLA/92/TEP/4
Emission Line Galaxies in the STIS Parallel Survey I: Observations and Data Analysis
In the first three years of operation STIS obtained slitless spectra of
approximately 2500 fields in parallel to prime HST observations as part of the
STIS Parallel Survey (SPS). The archive contains almost 300 fields at high
galactic latitude (|b|>30) with spectroscopic exposure times greater than 3000
seconds. This sample contains 220 fields (excluding special regions and
requiring a consistent grating angle) observed between 6 June 1997 and 21
September 2000, with a total survey area of about 160 square arcminutes. At
this depth, the SPS detects an average of one emission line galaxy per three
fields. We present the analysis of these data, and the identification of 131
low to intermediate redshift galaxies detected by optical emission lines. The
sample contains 78 objects with emission lines that we infer to be redshifted
[OII]3727 emission at 0.43<z<1.7. The comoving number density of these objects
is comparable to that of H-alpha emitting galaxies in the NICMOS parallel
observations. One quasar and three probable Seyfert galaxies are detected. Many
of the emission-line objects show morphologies suggestive of mergers or
interactions. The reduced data are available upon request from the authors.Comment: 58 preprint pages, including 26 figures; accepted for publication in
ApJ
Masses and Decay Constants of Heavy-Light Mesons Using the Multistate Smearing Technique
We present results for f_B and masses of low-lying heavy-light mesons.
Calculations were performed in the quenched approximation using multistate
smearing functions generated from a spinless relativistic quark model
Hamiltonian. Beta values range from 5.7 to 6.3, and light quark masses
corresponding to pion masses as low as 300 MeV are computed at each value. We
use the 1P--1S charmonium splitting to set the overall scale.Comment: 9 pages, 13 figures, and 5 tables as a single 193K compressed and
uuencoded Postscript file, FERMILAB--CONF--93/376-
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