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NIHAO XVI: the properties and evolution of kinematically selected discs, bulges, and stellar haloes

MPS-Authors

Obreja,  Aura
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Dutton,  Aaron A.
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Macciò,  Andrea V.
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Moster,  Benjamin
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Buck,  Tobias
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

van den Ven,  Glenn
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Wang,  Liang
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Stinson,  Gregory S.
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

Zhu,  Ling
Max Planck Institute for Astronomy, Max Planck Society and Cooperation Partners;

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Citation

Obreja, A., Dutton, A. A., Macciò, A. V., Moster, B., Buck, T., van den Ven, G., et al. (2019). NIHAO XVI: the properties and evolution of kinematically selected discs, bulges, and stellar haloes. Monthly Notices of the Royal Astronomical Society, 487, 4424-4456.


Cite as: https://hdl.handle.net/21.11116/0000-0005-D034-5
Abstract
We use 25 simulated galaxies from the NIHAO project to define and characterize a variety of kinematic stellar structures: thin and thick discs, large-scale single discs, classical and pseudo-bulges, spheroids, inner discs, and stellar haloes. These structures have masses, spins, shapes, and rotational support in good agreement with theoretical expectations and observational data. Above a dark matter halo mass of 2.5× 10^ 11 M_{\odot }, all galaxies have a classical bulge and 70 per cent have a thin and thick disc. The kinematic (thin) discs follow a power-law relation between angular momentum and stellar mass J_*=3.4M_*^{1.26± 0.06}, in very good agreement with the prediction based on the empirical stellar-to-halo-mass relation in the same mass range, and show a strong correlation between maximum `observed' rotation velocity and dark matter halo circular velocity v_c=6.4v_max^{0.64± 0.04}. Tracing back in time these structures' progenitors, we find all of them to lose a fraction 1 - fj of their maximum angular momentum. Thin discs are significantly better at retaining their high- redshift spins (fj ̃ 0.70) than thick ones (fj ̃ 0.40). Stellar haloes have their progenitor baryons assembled the latest (z1/2 ̃ 1.1) and over the longest time-scales (τ ̃ 6.2 Gyr), and have the smallest fraction of stars born in situ (fin situ = 0.35 ± 0.14). All other structures have 1.5 ≲ z1/2 ≲ 3, τ = 4 ± 2 Gyr, and fin situ ≳ 0.9.