1,075 research outputs found

    Simulating cosmic metal enrichment by the first galaxies

    Get PDF
    We study cosmic metal enrichment via AMR hydrodynamical simulations in a (10 Mpc/h)3^3 volume following the Pop III-Pop II transition and for different Pop III IMFs. We have analyzed the joint evolution of metal enrichment on galactic and intergalactic scales at z=6 and z=4. Galaxies account for <9% of the baryonic mass; the remaining gas resides in the diffuse phases: (a) voids, i.e. regions with extremely low density (Δ\Delta<1), (b) the true intergalactic medium (IGM, 1<Δ\Delta<10) and (c) the circumgalactic medium (CGM, 10<Δ<102.5\Delta<10^{2.5}), the interface between the IGM and galaxies. By z=6 a galactic mass-metallicity relation is established. At z=4, galaxies with a stellar mass M=108.5MM_*=10^{8.5}M_\odot show log(O/H)+12=8.19, consistent with observations. The total amount of heavy elements rises from ΩZSFH=1.52106\Omega^{SFH}_Z=1.52\, 10^{-6} at z=6 to 8.05 10610^{-6} at z=4. Metals in galaxies make up to ~0.89 of such budget at z=6; this fraction increases to ~0.95 at z=4. At z=6 (z=4) the remaining metals are distributed in CGM/IGM/voids with the following mass fractions: 0.06/0.04/0.01 (0.03/0.02/0.01). Analogously to galaxies, at z=4 a density-metallicity (Δ\Delta-Z) relation is in place for the diffuse phases: the IGM/voids have a spatially uniform metallicity, Z~103.510^{-3.5}Zsun; in the CGM Z steeply rises with density up to ~10210^{-2}Zsun. In all diffuse phases a considerable fraction of metals is in a warm/hot (T>104.510^{4.5}K) state. Due to these physical conditions, CIV absorption line experiments can probe only ~2% of the total carbon present in the IGM/CGM; however, metal absorption line spectra are very effective tools to study reionization. Finally, the Pop III star formation history is almost insensitive to the chosen Pop III IMF. Pop III stars are preferentially formed in truly pristine (Z=0) gas pockets, well outside polluted regions created by previous star formation episodes.Comment: 23 pages, 18 figures, 3 tables, Accepted for publication in MNRA

    Manejo integrado de corós em trigo e culturas associadas.

    Get PDF
    bitstream/CNPT-2010/40568/1/p-co203.pd

    The stellar populations of high-redshift dwarf galaxies

    Full text link
    We use high-resolution (10\approx 10 pc), zoom-in simulations of a typical (stellar mass M1010MM_\star\simeq10^{10}M_\odot) Lyman Break Galaxy (LBG) at z6z\simeq 6 to investigate the stellar populations of its six dwarf galaxy satellites, whose stellar [gas] masses are in the range log(M/M)69\log (M_\star/M_\odot) \simeq 6-9 [log(Mgas/M)4.37.75\log (M_{gas}/M_\odot) \simeq4.3-7.75]. The properties and evolution of satellites show no dependence on the distance from the central massive LBG (<11.5< 11.5 kpc). Instead, their star formation and chemical enrichment histories are tightly connected their stellar (and sub-halo) mass. High-mass dwarf galaxies (M5×108M\rm M_\star \gtrsim 5\times 10^8 M_\odot) experience a long history of star formation, characterised by many merger events. Lower-mass systems go through a series of short star formation episodes, with no signs of mergers; their star formation activity starts relatively late (z7z\approx 7), and it is rapidly quenched by internal stellar feedback. In spite of the different evolutionary patterns, all satellites show a spherical morphology, with ancient and more metal-poor stars located towards the inner regions. All six dwarf satellites experienced high star formation rate (>5Myr1\rm >5\,M_\odot yr ^{-1}) bursts, which can be detected by JWST while targeting high-zz LBGs.Comment: 17 pages, 14 figures. To be published in MNRA
    corecore