2009
DOI: 10.1017/s1743921310002863
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Modeling high-redshift galaxies: what can we learn from high and ultra-high resolution hydrodynamical simulations?

Abstract: Abstract. We present results from a high resolution cosmological galaxy formation simulation called Mare Nostrum and a ultra-high resimulation of the first 500 million years of a single, Milky Way (MW) sized galaxy. Using the cosmological run, we measure UV luminosity functions and assess their sensitivity to both cosmological parameters and dust extinction. We find remarkably good agreement with the existing data over the redshift range 4 < z < 7 provided we adopt the favoured cosmology (WMAP 5 year parameter… Show more

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Cited by 2 publications
(2 citation statements)
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“…The Nut Simulation † is an ultra-high resolution cosmological simulation of a Milky Way like galaxy forming at the intersection of 3 filaments in a ΛCDM cosmology (Slyz et al 2009;Devriendt et al 2010). We perform the simulation with ramses (Teyssier 2002) including cooling, a UV background (Haardt & Madau 1996), SF and SN feedback with metal enrichment (Dubois & Teyssier 2008) achieving a maximum physical spatial resolution of ≈ 0.5pc in the densest regions at all times.…”
Section: Star Formation During Cold-mode Accretion and The Onset Of Amentioning
confidence: 99%
See 1 more Smart Citation
“…The Nut Simulation † is an ultra-high resolution cosmological simulation of a Milky Way like galaxy forming at the intersection of 3 filaments in a ΛCDM cosmology (Slyz et al 2009;Devriendt et al 2010). We perform the simulation with ramses (Teyssier 2002) including cooling, a UV background (Haardt & Madau 1996), SF and SN feedback with metal enrichment (Dubois & Teyssier 2008) achieving a maximum physical spatial resolution of ≈ 0.5pc in the densest regions at all times.…”
Section: Star Formation During Cold-mode Accretion and The Onset Of Amentioning
confidence: 99%
“…SF in the galaxy, its satellites and haloes embedded in the filaments results in many SN explosions, which are individually resolved. The numerous bubbles overlap, creating an extended cavity through which the hot gas escapes the galactic potential in the form of a wind (see Slyz et al 2009;Devriendt et al 2010, for figures illustrating this and additional technical details). By z = 9, when the dark matter halo mass has reached ∼ 10 9 M , the wind extends to ≈ 6r vir , filling the virial sphere with hot, diffuse gas not unlike the shock-heated gaseous halo found in galaxies above the mass threshold for a stable virial shock (e.g.…”
Section: Star Formation During Cold-mode Accretion and The Onset Of Amentioning
confidence: 99%