The origin of accreted stellar halo populations in the milky way using apogee, gaia, and the eagle simulations
dc.contributor.author | Mackereth, J. Ted | |
dc.contributor.author | Schiavon, Ricardo P. | |
dc.contributor.author | Pfeffer, Joel | |
dc.contributor.author | Hayes, Christian R. | |
dc.contributor.author | Bovy, Jo | |
dc.contributor.author | Anguiano, Borja | |
dc.contributor.author | Prieto, Carlos Allende | |
dc.contributor.author | Hasselquist, Sten | |
dc.contributor.author | Holtzman, Jon | |
dc.contributor.author | Johnson, Jennifer A. | |
dc.contributor.author | Majewski, Steven R. | |
dc.contributor.author | O’Connell, Robert | |
dc.contributor.author | Shetrone, Matthew | |
dc.contributor.author | Tissera, Patricia B. | |
dc.contributor.author | Fernandez-Trincado, J. G. | |
dc.date.accessioned | 2023-06-07T14:22:21Z | |
dc.date.available | 2023-06-07T14:22:21Z | |
dc.date.issued | 2019-01-21 | |
dc.description | Indexación Scopus | es |
dc.description.abstract | Kinematics of halo stars. We show that ∼2/3 of nearby halo stars have high orbital eccentricities (e 0.8), and abundance patterns typical of massive Milky Way dwarf galaxy satellites today, characterized by relatively low [Fe/H], [Mg/Fe], [Al/Fe], and [Ni/Fe]. The trend followed by high-e stars in the [Mg/Fe]-[Fe/H] plane shows a change of slope at [Fe/H] ∼ -1.3, which is also typical of stellar populations from relatively massive dwarf galaxies. Low-e stars exhibit no such change of slope within the observed [Fe/H] range and show slightly higher abundances of Mg, Al, and Ni. Unlike their low-e counterparts, high-e stars show slightly retrograde motion, make higher vertical excursions, and reach larger apocentre radii. By comparing the position in [Mg/Fe]-[Fe/H] space of high-e stars with those of accreted galaxies from the EAGLE suite of cosmological simulations, we constrain the mass of the accreted satellite to be in the range 108.5≲ M ≲ 109M⊙ We show that the median orbital eccentricities of debris are largely unchanged since merger time, implying that this accretion event likely happened at z≲1.5. The exact nature of the low-e population is unclear, but we hypothesize that it is a combination of in situ star formation, high-|z| disc stars, lower mass accretion events, and contamination by the low-e tail of the high-e population. Finally, our results imply that the accretion history of the Milky Way was quite unusual. | es |
dc.identifier.citation | Monthly Notices of the Royal Astronomical Society Volume 482, Issue 3, Pages 3426 - 3442 21 January 2019 | es |
dc.identifier.doi | 10.1093/mnras/sty2955 | en |
dc.identifier.issn | 0035-8711 | |
dc.identifier.uri | https://repositorio.unab.cl/xmlui/handle/ria/50409 | |
dc.language.iso | en | es |
dc.publisher | Monthly Notices of the Royal Astronomical Society | es |
dc.rights.license | Attribution 4.0 International (CC BY 4.0) | en |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en |
dc.subject | Galaxy | es |
dc.subject | Galaxy: abundances | es |
dc.subject | Galaxy: formation | es |
dc.subject | Galaxy: halo | es |
dc.subject | Kinematics and dynamics | es |
dc.subject | Stellar content | es |
dc.title | The origin of accreted stellar halo populations in the milky way using apogee, gaia, and the eagle simulations | es |
dc.type | Artículo | es |
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