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  • 1
    Publication Date: 2015-09-16
    Description: The instantaneous H i content of galaxies is thought to be governed by recent accretion and environment. We examine these effects within a cosmological hydrodynamic simulation that includes a heuristic galactic outflow model that reproduces basic observed trends of H i in galaxies. We show that this model reproduces the observed H i mass function in bins of stellar mass, as well as the H i richness ( $M_{\rm H\,\small {I}}$ / M * ) versus local galaxy density. For satellite galaxies in massive ( 10 12 M ) haloes, the H i richness distribution is bimodal and the median drops towards the largest halo masses. The depletion time-scale of H i entering a massive halo is more rapid, in contrast to the specific star formation rate which shows little variation in the attenuation rate versus halo mass. This suggests that, up to the halo mass scales probed here ( 10 14 M ), star formation is mainly attenuated by starvation, but H i is additionally removed by stripping once a hot gaseous halo is present. In low-mass haloes, the H i richness of satellites is independent of radius, while in very massive haloes they become gas-poor towards the centre, confirming the increasing strength of the stripping with halo mass. Mergers somewhat increase the H i richness and its scatter about the mean relation, tracking the metallicity in a way consistent with it arising from inflow fluctuations, while star formation is significantly boosted relative to H i .
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 2
    Publication Date: 2015-09-27
    Description: The instantaneous H i content of galaxies is thought to be governed by recent accretion and environment. We examine these effects within a cosmological hydrodynamic simulation that includes a heuristic galactic outflow model that reproduces basic observed trends of H i in galaxies. We show that this model reproduces the observed H i mass function in bins of stellar mass, as well as the H i richness ( $M_{\rm H\,\small {I}}$ / M * ) versus local galaxy density. For satellite galaxies in massive ( 10 12 M ) haloes, the H i richness distribution is bimodal and the median drops towards the largest halo masses. The depletion time-scale of H i entering a massive halo is more rapid, in contrast to the specific star formation rate which shows little variation in the attenuation rate versus halo mass. This suggests that, up to the halo mass scales probed here ( 10 14 M ), star formation is mainly attenuated by starvation, but H i is additionally removed by stripping once a hot gaseous halo is present. In low-mass haloes, the H i richness of satellites is independent of radius, while in very massive haloes they become gas-poor towards the centre, confirming the increasing strength of the stripping with halo mass. Mergers somewhat increase the H i richness and its scatter about the mean relation, tracking the metallicity in a way consistent with it arising from inflow fluctuations, while star formation is significantly boosted relative to H i .
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 3
    Publication Date: 2006-04-15
    Print ISSN: 0021-8979
    Electronic ISSN: 1089-7550
    Topics: Physics
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  • 4
    Publication Date: 2014-05-12
    Print ISSN: 0027-8424
    Electronic ISSN: 1091-6490
    Topics: Biology , Medicine , Natural Sciences in General
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  • 5
    Publication Date: 2016-06-14
    Description: We introduce a series of 20 cosmological hydrodynamical simulations of L * ( M 200 = 10 11.7 –10 12.3 M ) and group-sized ( M 200 = 10 12.7 –10 13.3 M ) haloes run with the model used for the eagle project, which additionally includes a non-equilibrium ionization and cooling module that follows 136 ions. The simulations reproduce the observed correlation, revealed by COS-Halos at z ~ 0.2, between ${{\rm O} \small{VI}}$ column density at impact parameters b 〈 150 kpc and the specific star formation rate (sSFR  SFR/ M * ) of the central galaxy at z ~ 0.2. We find that the column density of circumgalactic ${O \small {VI}}$ is maximal in the haloes associated with L * galaxies, because their virial temperatures are close to the temperature at which the ionization fraction of ${O \small {VI}}$ peaks ( T ~ 10 5.5  K). The higher virial temperature of group haloes (〉10 6  K) promotes oxygen to higher ionization states, suppressing the ${O \small {VI}}$ column density. The observed $N_{\rm O\,\small {VI}}$ –sSFR correlation therefore does not imply a causal link, but reflects the changing characteristic ionization state of oxygen as halo mass is increased. In spite of the mass dependence of the oxygen ionization state, the most abundant circumgalactic oxygen ion in both L * and group haloes is ${O\,{\small VII}}$ ; ${O \small {VI}}$ accounts for only 0.1 per cent of the oxygen in group haloes and 0.9–1.3 per cent with L * haloes. Nonetheless, the metals traced by ${O \small {VI}}$ absorbers represent a fossil record of the feedback history of galaxies over a Hubble time; their characteristic epoch of ejection corresponds to z 〉 1 and much of the ejected metal mass resides beyond the virial radius of galaxies. For both L * and group galaxies, more of the oxygen produced and released by stars in the circumgalactic medium (within twice the virial radius) than in the stars and interstellar medium of the galaxy.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 6
    Publication Date: 2016-01-16
    Description: The thermal and chemical properties of the hot diffuse intragroup medium (IGrM) provide important constraints on the feedback processes associated with massive galaxy formation and evolution. Here we explore these constraints via a detailed analysis of the global properties of simulated z  〈 3 galaxy groups drawn from a cosmological simulation that includes a well-constrained prescription for momentum-driven, stellar/supernova-powered galactic outflows but no active galactic nucleus (AGN) feedback. Our simulation successfully reproduces the key observed IGrM properties, including X-ray trends, for all but the most massive groups. The z  〈 1 redshift evolution of these is also consistent with the observations. Contrary to expectations, the simulated groups’ IGrM does not suffer catastrophic cooling. Yet, the z  = 0 group stellar mass is ~2 x  too large. We show that this is due to the build-up of cold gas in the massive galaxies before they are incorporated inside groups. This indicates that other feedback mechanisms must activate in real galaxies once they grow to M * a few  x 10 10 M and that these must be powerful enough to expel a significant fraction of the gas from the galactic haloes. Gentle ‘maintenance-mode’ AGN feedback would be insufficient to bring the stellar and baryonic fractions into agreement with the observations. Just as importantly, we find that the stellar/supernova-powered winds are essential for understanding the IGrM metal abundances. Our simulation is able to reproduce the observed relationship between the global IGrM iron and silicon abundances and the group X-ray temperature, and these results should be relatively insensitive to the addition of AGN feedback.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 7
    Publication Date: 2014-08-30
    Description: We examine how H i and metal absorption lines within low-redshift galaxy haloes trace the dynamical state of circumgalactic gas, using cosmological hydrodynamic simulations that include a well-vetted heuristic model for galactic outflows. We categorize inflowing, outflowing, and ambient gas based on its history and fate as tracked in our simulation. Following our earlier work, showing that the ionization level of absorbers was a primary factor in determining the physical conditions of absorbing gas, we show here that it is also a governing factor for its dynamical state. Low-ionization metal absorbers (e.g. Mg ii ) tend to arise in gas that will fall on to galaxies within several Gyr, while high-ionization metal absorbers (e.g. O vi ) generally trace material that was deposited by outflows many Gyr ago. Inflowing gas is dominated by enriched material that was previously ejected in an outflow; hence, accretion at low redshifts is typically substantially enriched. Recycling wind material is preferentially found closer to galaxies, and is more dominant in lower mass haloes since high-mass haloes have more hot gas that is able to support itself against infall. Low-mass haloes also tend to re-eject more of their accreted material, owing to our outflow prescription that employs higher mass loading factors for lower mass galaxies. Typical H i absorbers trace unenriched ambient material that is not participating in the baryon cycle, but stronger H i absorbers arise in cool, enriched inflowing gas. Instantaneous radial velocity measures of absorbers are generally poor at distinguishing between inflowing and outflowing gas, except in the case of very recent outflows. These results suggest that probing halo gas using a range of absorbers can provide detailed information about the amount and physical conditions of material that is participating in the baryon cycle.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 8
    Publication Date: 2014-09-03
    Description: The Gemini Planet Imager is a dedicated facility for directly imaging and spectroscopically characterizing extrasolar planets. It combines a very high-order adaptive optics system, a diffraction-suppressing coronagraph, and an integral field spectrograph with low spectral resolution but high spatial resolution. Every aspect of the Gemini Planet Imager has been tuned...
    Keywords: Exoplanets Special Feature
    Print ISSN: 0027-8424
    Electronic ISSN: 1091-6490
    Topics: Biology , Medicine , Natural Sciences in General
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  • 9
    Publication Date: 2015-01-10
    Description: Observations suggest that C ii was more abundant than C iv in the intergalactic medium towards the end of the hydrogen reionization epoch ( z  ~ 6). This transition provides a unique opportunity to study the enrichment history of intergalactic gas and the growth of the ionizing ultraviolet background (UVB) at early times. We study how carbon absorption evolves from z  = 10 to 5 using a cosmological hydrodynamic simulation that includes a self-consistent multifrequency UVB as well as a well-constrained model for galactic outflows to disperse metals. Our predicted UVB is within ~2–4 times of that from Haardt & Madau, which is fair agreement given the uncertainties. Nonetheless, we use a calibration in post-processing to account for Lyman α forest measurements while preserving the predicted spectral slope and inhomogeneity. The UVB fluctuates spatially in such a way that it always exceeds the volume average in regions where metals are found. This implies both that a spatially uniform UVB is a poor approximation and that metal absorption is not sensitive to the epoch when H ii regions overlap globally even at column densities of 10 12  cm –2 . We find, consistent with observations, that the C ii mass fraction drops to low redshift while C iv rises owing the combined effects of a growing UVB and continued addition of carbon in low-density regions. This is mimicked in absorption statistics, which broadly agree with observations at z  = 6–3 while predicting that the absorber column density distributions rise steeply to the lowest observable columns. Our model reproduces the large observed scatter in the number of low-ionization absorbers per sightline, implying that the scatter does not indicate a partially neutral Universe at z  ~ 6.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 10
    Publication Date: 2014-04-19
    Description: An accurate treatment of the multiphase interstellar medium (ISM) in hydrodynamic galaxy simulations requires that we follow not only the thermal evolution of the gas, but also the evolution of its chemical state, including its molecular chemistry, without assuming chemical (including ionization) equilibrium. We present a reaction network that can be used to solve for this thermo-chemical evolution. Our model follows the evolution of all ionization states of the 11 elements that dominate the cooling rate, along with important molecules such as H 2 and CO, and the intermediate molecular species that are involved in their formation (20 molecules in total). We include chemical reactions on dust grains, thermal processes involving dust, cosmic ray ionization and heating and photochemical reactions. We focus on conditions typical for the diffuse ISM, with densities of 10 –2 cm –3 n H 10 4 cm –3 and temperatures of 10 2 K T 10 4 K, and we consider a range of radiation fields, including no UV radiation. In this paper, we consider only gas that is optically thin, while paper II considers gas that becomes shielded from the radiation field. We verify the accuracy of our model by comparing chemical abundances and cooling functions in chemical equilibrium with the photoionization code cloudy . We identify the major coolants in diffuse interstellar gas to be C ii , Si ii and Fe ii , along with O i and H 2 at densities n H 10 2 cm –3 . Finally, we investigate the impact of non-equilibrium chemistry on the cooling functions of isochorically or isobarically cooling gas. We find that, at T  〈 10 4  K, recombination lags increase the electron abundance above its equilibrium value at a given temperature, which can enhance the cooling rate by up to two orders of magnitude. The cooling gas also shows lower H 2 abundances than in equilibrium, by up to an order of magnitude.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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