5 results on '"van de Voort F"'
Search Results
2. Predictions for the angular dependence of gas mass flow rate and metallicity in the circumgalactic medium
- Author
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Mark Vogelsberger, Freeke van de Voort, Annalisa Pillepich, Celine Peroux, Federico Marinacci, Dylan Nelson, Lars Hernquist, Peroux C., Nelson D., Van De Voort F., Pillepich A., Marinacci F., Vogelsberger M., Hernquist L., Laboratoire d'Astrophysique de Marseille (LAM), Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS), MIT Kavli Institute for Astrophysics and Space Research, and Massachusetts Institute of Technology. Department of Physics
- Subjects
Physics ,Stellar mass ,Metallicity ,FOS: Physical sciences ,Astronomy and Astrophysics ,Observable ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Galaxy ,methods: numerical ,galaxies: haloes ,quasars: absorption lines ,Azimuth ,galaxies: haloe ,galaxies: abundance ,[SDU]Sciences of the Universe [physics] ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,Mass flow rate ,galaxies: formation ,Outflow ,galaxies: evolution ,Astrophysics::Galaxy Astrophysics ,Order of magnitude - Abstract
We use cosmological hydrodynamical simulations to examine the physical properties of the gas in the circumgalactic media (CGM) of star-forming galaxies as a function of angular orientation. We utilise TNG50 of the IllustrisTNG project, as well as the EAGLE simulation to show that observable properties of CGM gas correlate with azimuthal angle, defined as the galiocentric angle with respect to the central galaxy. Both simulations are in remarkable agreement in predicting a strong modulation of flow rate direction with azimuthal angle: inflow is more substantial along the galaxy major axis, while outflow is strongest along the minor axis. The absolute rates are noticeably larger for higher (log(M_* / M_sun) ~ 10.5) stellar mass galaxies, up to an order of magnitude compared to M^dot < 1 M_sun/yr/sr for log(M_* / M_sun) ~ 9.5 objects. Notwithstanding the different numerical and physical models, both TNG50 and EAGLE predict that the average metallicity of the CGM is higher along the minor versus major axes of galaxies. The angular signal is robust across a wide range of galaxy stellar mass 8.5 < log(M_* / M_sun) < 10.5 at z 100 kpc. Our results present a global picture whereby, despite the numerous mixing processes, there is a clear angular dependence of the CGM metallicity. We make forecasts for future large survey programs that will be able to compare against these expectations. Indeed, characterising the kinematics, spatial distribution and metal content of CGM gas is key to a full understanding of the exchange of mass, metals, and energy between galaxies and their surrounding environments., Accepted for publication in MNRAS; 13 pages, 6 figures
- Published
- 2020
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3. Neutron star mergers and rare core-collapse supernovae as sources of r-process enrichment in simulated galaxies
- Author
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Federico Marinacci, Rüdiger Pakmor, Robert J. J. Grand, Facundo A. Gómez, Volker Springel, Freeke van de Voort, Van De Voort F., Pakmor R., Grand R.J.J., Springel V., Gomez F.A., and Marinacci F.
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Metallicity ,Milky Way ,FOS: Physical sciences ,galaxies: Dwarf ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,methods: Numerical ,Astrophysics::Solar and Stellar Astrophysics ,stars: Abundance ,Solar and Stellar Astrophysics (astro-ph.SR) ,Astrophysics::Galaxy Astrophysics ,Dwarf galaxy ,High Energy Astrophysical Phenomena (astro-ph.HE) ,Physics ,Galaxy: Abundance ,Astronomy and Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Galaxy ,Neutron star ,Supernova ,Stars ,Astrophysics - Solar and Stellar Astrophysics ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,stars: Neutron ,r-process ,supernovae: General ,Astrophysics - High Energy Astrophysical Phenomena - Abstract
We use cosmological, magnetohydrodynamical simulations of Milky Way-mass galaxies from the Auriga project to study their enrichment with rapid neutron capture (r-process) elements. We implement a variety of enrichment models from both binary neutron star mergers and rare core-collapse supernovae. We focus on the abundances of (extremely) metal-poor stars, most of which were formed during the first ~Gyr of the Universe in external galaxies and later accreted onto the main galaxy. We find that the majority of metal-poor stars are r-process enriched in all our enrichment models. Neutron star merger models result in a median r-process abundance ratio which increases with metallicity, whereas the median trend in rare core-collapse supernova models is approximately flat. The scatter in r-process abundance increases for models with longer delay times or lower rates of r-process producing events. Our results are nearly perfectly converged, in part due to the mixing of gas between mesh cells in the simulations. Additionally, different Milky Way-mass galaxies show only small variation in their respective r-process abundance ratios. Current (sparse and potentially biased) observations of metal-poor stars in the Milky Way seem to prefer rare core-collapse supernovae over neutron star mergers as the dominant source of r-process elements at low metallicity, but we discuss possible caveats to our models. Dwarf galaxies which experience a single r-process event early in their history show highly enhanced r-process abundances at low metallicity, which is seen both in observations and in our simulations. We also find that the elements produced in a single event are mixed with ~10^8 Msun of gas relatively quickly, distributing the r-process elements over a large region., Accepted for publication in MNRAS. Revised version: added Figure 13 (on mixing of iron and r-process elements) and an Appendix (on iron and magnesium abundances) and updated the r-process yields (Tables 1 and 2 and normalization of abundances)
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- 2020
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4. Magnetizing the circumgalactic medium of disc galaxies
- Author
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Facundo A. Gómez, Christine M. Simpson, Freeke van de Voort, Federico Marinacci, Rüdiger Pakmor, Thomas Guillet, Robert J. J. Grand, Christoph Pfrommer, Volker Springel, Rebekka Bieri, Pakmor R., Van De Voort F., Bieri R., Gomez F.A., Grand R.J.J., Guillet T., Marinacci F., Pfrommer C., Simpson C.M., and Springel V.
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MHD ,FOS: Physical sciences ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Disc galaxy ,01 natural sciences ,methods: numerical ,galaxies: haloe ,0103 physical sciences ,Galaxy formation and evolution ,010303 astronomy & astrophysics ,Astrophysics::Galaxy Astrophysics ,Physics ,010308 nuclear & particles physics ,Astronomy and Astrophysics ,Astrophysics - Astrophysics of Galaxies ,Accretion (astrophysics) ,Galaxy ,Redshift ,Magnetic field ,Galaxy: formation ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,galaxies: magnetic field ,Magnetohydrodynamics ,Dynamo - Abstract
The circumgalactic medium (CGM) is one of the frontiers of galaxy formation and intimately connected to the galaxy via accretion of gas on to the galaxy and gaseous outflows from the galaxy. Here we analyse the magnetic field in the CGM of the Milky Way-like galaxies simulated as part of the \textsc{Auriga} project that constitutes a set of high resolution cosmological magnetohydrodynamical zoom simulations. We show that before $z=1$ the CGM becomes magnetised via galactic outflows that transport magnetised gas from the disk into the halo. At this time the magnetisation of the CGM closely follows its metal enrichment. We then show that at low redshift an in-situ turbulent dynamo that operates on a timescale of Gigayears further amplifies the magnetic field in the CGM and saturates before $z=0$. The magnetic field strength reaches a typical value of $0.1\,\mu G$ at the virial radius at $z=0$ and becomes mostly uniform within the virial radius. Its Faraday rotation signal is in excellent agreement with recent observations. For most of its evolution the magnetic field in the CGM is an unordered small scale field. Only strong coherent outflows at low redshift are able to order the magnetic field in parts of the CGM that are directly displaced by these outflows., Comment: 14 pages, 15 figures, accepted by MNRAS, updated Fig. 15 in proofs with errorbars
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5. The origin of the diverse morphologies and kinematics of Milky Way-mass galaxies in the FIRE-2 simulations.
- Author
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Garrison-Kimmel S, Hopkins PF, Wetzel A, El-Badry K, Sanderson RE, Bullock JS, Ma X, van de Voort F, Hafen Z, Faucher-Giguère CA, Hayward CC, Quataert E, Kereš D, and Boylan-Kolchin M
- Abstract
We use hydrodynamic cosmological zoom-in simulations from the Feedback in Realistic Environments project to explore the morphologies and kinematics of 15 Milky Way (MW)-mass galaxies. Our sample ranges from compact, bulge-dominated systems with 90 per cent of their stellar mass within 2.5 kpc to well-ordered discs that reach ≳15 kpc. The gas in our galaxies always forms a thin, rotation-supported disc at z = 0, with sizes primarily determined by the gas mass. For stars, we quantify kinematics and morphology both via the fraction of stars on disc-like orbits and with the radial extent of the stellar disc. In this mass range, stellar morphology and kinematics are poorly correlated with the properties of the halo available from dark matter-only simulations (halo merger history, spin, or formation time). They more strongly correlate with the gaseous histories of the galaxies: those that maintain a high gas mass in the disc after z ~ 1 develop well-ordered stellar discs. The best predictor of morphology we identify is the spin of the gas in the halo at the time the galaxy formed 1/2 of its stars (i.e. the gas that builds the galaxy). High- z mergers, before a hot halo emerges, produce some of the most massive bulges in the sample (from compact discs in gas-rich mergers), while later-forming bulges typically originate from internal processes, as satellites are stripped of gas before the galaxies merge. Moreover, most stars in z = 0 MW-mass galaxies (even z = 0 bulge stars) form in a disc: ≳60-90 per cent of stars begin their lives rotationally supported.
- Published
- 2018
- Full Text
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