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Co-formation of the disc and the stellar halo★

Vasily BelokurovCenter for Computational Astrophysics, Flatiron Institute, 162 5th Avenue, New York, NY 10010, USADenis ErkalDepartment of Physics, University of Surrey, Guildford GU2 7XHN. W. EvansInstitute of Astronomy, Madingley Road, Cambridge CB3 0HAS. E. KoposovDepartment of Physics, McWilliams Center for Cosmology, Carnegie Mellon University, 5000 Forbes Avenue, Pittsburgh, PA 15213, USAAlis J. DeasonInstitute for Computational Cosmology, Department of Physics, University of Durham, South Road, Durham DH1 3LE, UK
2018en
ABI

Аннотация

Using a large sample of main sequence stars with 7D measurements supplied by Gaia and SDSS, we study the kinematic properties of the local (within 10 kpc from the Sun) stellar halo. We demonstrate that the halo's velocity ellipsoid evolves strongly with metallicity. At the low-[Fe/H] end, the orbital anisotropy (the amount of motion in the radial direction compared with the tangential one) is mildly radial, with 0.2 << 0.4. For stars with [Fe/H] > -1.7, however, we measure extreme values of 0.9. Across the metallicity range considered, namely -3 < [Fe/H] < -1, the stellar halo's spin is minimal, at the level of 20 < v (kms -1 ) < 30. Using a suite of cosmological zoom-in simulations of halo formation, we deduce that the observed acute anisotropy is inconsistent with the continuous accretion of dwarf satellites. Instead, we argue, the stellar debris in the inner halo was deposited in a major accretion event by a satellite with M vir > 10 10 M around the epoch of the Galactic disc formation, between 8 and 11 Gyr ago. The radical halo anisotropy is the result of the dramatic radialization of the massive progenitor's orbit, amplified by the action of the growing disc.

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